[76897] |
Title: Single-sided magnetic particle imaging: magnetic field and gradient. |
Written by: K. Gräfe, M. Grüttner, T.F. Sattel, M. Graeser, and T.M. Buzug |
in: <em>Proc. {SPIE}</em>. (2013). |
Volume: <strong>8672</strong>. Number: |
on pages: |
Chapter: |
Editor: |
Publisher: |
Series: |
Address: |
Edition: |
ISBN: |
how published: |
Organization: |
School: |
Institution: |
Type: |
DOI: 10.1117/12.2001610 |
URL: http://dx.doi.org/10.1117/12.2001610 |
ARXIVID: |
PMID: |
Note: inproceedings, Paper ID: 867219
Abstract: {Magnetic Particle Imaging} ({MPI}) has been presented by Gleich and Weizenecker in 2005. Since then, a number of innovations have been introduced by many di erent research groups. In 2009, for instance, Sattel et al. presented a novel single-sided {MPI} scanner geometry. The major advantage of this particular scanner geometry is the unlimited measurement eld. For the imaging process in {MPI}, super-paramagnetic iron oxide nanoparticles ({SPIONs}) are applied as tracer material. The tracer is excited by sinusoidally varying magnetic elds. In this contribution, simulated magnetic elds were evaluated based on the measured eld distribution of a single-sided scanner realization. It is of particular importance to know the quality of the gradient elds, since image resolution in {MPI} is directly linked to the gradient strength.
[76897] |
Title: Single-sided magnetic particle imaging: magnetic field and gradient. |
Written by: K. Gräfe, M. Grüttner, T.F. Sattel, M. Graeser, and T.M. Buzug |
in: <em>Proc. {SPIE}</em>. (2013). |
Volume: <strong>8672</strong>. Number: |
on pages: |
Chapter: |
Editor: |
Publisher: |
Series: |
Address: |
Edition: |
ISBN: |
how published: |
Organization: |
School: |
Institution: |
Type: |
DOI: 10.1117/12.2001610 |
URL: http://dx.doi.org/10.1117/12.2001610 |
ARXIVID: |
PMID: |
Note: inproceedings, Paper ID: 867219
Abstract: {Magnetic Particle Imaging} ({MPI}) has been presented by Gleich and Weizenecker in 2005. Since then, a number of innovations have been introduced by many di erent research groups. In 2009, for instance, Sattel et al. presented a novel single-sided {MPI} scanner geometry. The major advantage of this particular scanner geometry is the unlimited measurement eld. For the imaging process in {MPI}, super-paramagnetic iron oxide nanoparticles ({SPIONs}) are applied as tracer material. The tracer is excited by sinusoidally varying magnetic elds. In this contribution, simulated magnetic elds were evaluated based on the measured eld distribution of a single-sided scanner realization. It is of particular importance to know the quality of the gradient elds, since image resolution in {MPI} is directly linked to the gradient strength.
[76897] |
Title: Single-sided magnetic particle imaging: magnetic field and gradient. |
Written by: K. Gräfe, M. Grüttner, T.F. Sattel, M. Graeser, and T.M. Buzug |
in: <em>Proc. {SPIE}</em>. (2013). |
Volume: <strong>8672</strong>. Number: |
on pages: |
Chapter: |
Editor: |
Publisher: |
Series: |
Address: |
Edition: |
ISBN: |
how published: |
Organization: |
School: |
Institution: |
Type: |
DOI: 10.1117/12.2001610 |
URL: http://dx.doi.org/10.1117/12.2001610 |
ARXIVID: |
PMID: |
Note: inproceedings, Paper ID: 867219
Abstract: {Magnetic Particle Imaging} ({MPI}) has been presented by Gleich and Weizenecker in 2005. Since then, a number of innovations have been introduced by many di erent research groups. In 2009, for instance, Sattel et al. presented a novel single-sided {MPI} scanner geometry. The major advantage of this particular scanner geometry is the unlimited measurement eld. For the imaging process in {MPI}, super-paramagnetic iron oxide nanoparticles ({SPIONs}) are applied as tracer material. The tracer is excited by sinusoidally varying magnetic elds. In this contribution, simulated magnetic elds were evaluated based on the measured eld distribution of a single-sided scanner realization. It is of particular importance to know the quality of the gradient elds, since image resolution in {MPI} is directly linked to the gradient strength.
[76897] |
Title: Single-sided magnetic particle imaging: magnetic field and gradient. |
Written by: K. Gräfe, M. Grüttner, T.F. Sattel, M. Graeser, and T.M. Buzug |
in: <em>Proc. {SPIE}</em>. (2013). |
Volume: <strong>8672</strong>. Number: |
on pages: |
Chapter: |
Editor: |
Publisher: |
Series: |
Address: |
Edition: |
ISBN: |
how published: |
Organization: |
School: |
Institution: |
Type: |
DOI: 10.1117/12.2001610 |
URL: http://dx.doi.org/10.1117/12.2001610 |
ARXIVID: |
PMID: |
Note: inproceedings, Paper ID: 867219
Abstract: {Magnetic Particle Imaging} ({MPI}) has been presented by Gleich and Weizenecker in 2005. Since then, a number of innovations have been introduced by many di erent research groups. In 2009, for instance, Sattel et al. presented a novel single-sided {MPI} scanner geometry. The major advantage of this particular scanner geometry is the unlimited measurement eld. For the imaging process in {MPI}, super-paramagnetic iron oxide nanoparticles ({SPIONs}) are applied as tracer material. The tracer is excited by sinusoidally varying magnetic elds. In this contribution, simulated magnetic elds were evaluated based on the measured eld distribution of a single-sided scanner realization. It is of particular importance to know the quality of the gradient elds, since image resolution in {MPI} is directly linked to the gradient strength.
[76897] |
Title: Single-sided magnetic particle imaging: magnetic field and gradient. |
Written by: K. Gräfe, M. Grüttner, T.F. Sattel, M. Graeser, and T.M. Buzug |
in: <em>Proc. {SPIE}</em>. (2013). |
Volume: <strong>8672</strong>. Number: |
on pages: |
Chapter: |
Editor: |
Publisher: |
Series: |
Address: |
Edition: |
ISBN: |
how published: |
Organization: |
School: |
Institution: |
Type: |
DOI: 10.1117/12.2001610 |
URL: http://dx.doi.org/10.1117/12.2001610 |
ARXIVID: |
PMID: |
Note: inproceedings, Paper ID: 867219
Abstract: {Magnetic Particle Imaging} ({MPI}) has been presented by Gleich and Weizenecker in 2005. Since then, a number of innovations have been introduced by many di erent research groups. In 2009, for instance, Sattel et al. presented a novel single-sided {MPI} scanner geometry. The major advantage of this particular scanner geometry is the unlimited measurement eld. For the imaging process in {MPI}, super-paramagnetic iron oxide nanoparticles ({SPIONs}) are applied as tracer material. The tracer is excited by sinusoidally varying magnetic elds. In this contribution, simulated magnetic elds were evaluated based on the measured eld distribution of a single-sided scanner realization. It is of particular importance to know the quality of the gradient elds, since image resolution in {MPI} is directly linked to the gradient strength.
[76897] |
Title: Single-sided magnetic particle imaging: magnetic field and gradient. |
Written by: K. Gräfe, M. Grüttner, T.F. Sattel, M. Graeser, and T.M. Buzug |
in: <em>Proc. {SPIE}</em>. (2013). |
Volume: <strong>8672</strong>. Number: |
on pages: |
Chapter: |
Editor: |
Publisher: |
Series: |
Address: |
Edition: |
ISBN: |
how published: |
Organization: |
School: |
Institution: |
Type: |
DOI: 10.1117/12.2001610 |
URL: http://dx.doi.org/10.1117/12.2001610 |
ARXIVID: |
PMID: |
Note: inproceedings, Paper ID: 867219
Abstract: {Magnetic Particle Imaging} ({MPI}) has been presented by Gleich and Weizenecker in 2005. Since then, a number of innovations have been introduced by many di erent research groups. In 2009, for instance, Sattel et al. presented a novel single-sided {MPI} scanner geometry. The major advantage of this particular scanner geometry is the unlimited measurement eld. For the imaging process in {MPI}, super-paramagnetic iron oxide nanoparticles ({SPIONs}) are applied as tracer material. The tracer is excited by sinusoidally varying magnetic elds. In this contribution, simulated magnetic elds were evaluated based on the measured eld distribution of a single-sided scanner realization. It is of particular importance to know the quality of the gradient elds, since image resolution in {MPI} is directly linked to the gradient strength.