2018
DOI: 10.1002/mrm.27563
|View full text |Cite
|
Sign up to set email alerts
|

Nyquist ghost correction of breast diffusion weighted imaging using referenceless methods

Abstract: Purpose Correction of Nyquist ghosts for single‐shot spin‐echo EPI using the standard 3‐line navigator often fails in breast DWI because of incomplete fat suppression, respiration, and greater B0 inhomogeneity. The purpose of this work is to compare the performance of the 3‐line navigator with 4 data‐driven methods termed “referenceless methods,” including 2 previously proposed in literature, 1 introduced in this work, and finally a combination of all 3, in breast DWI. Methods Breast DWI was acquired for 41 pa… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
20
0

Year Published

2020
2020
2024
2024

Publication Types

Select...
7

Relationship

1
6

Authors

Journals

citations
Cited by 8 publications
(20 citation statements)
references
References 24 publications
0
20
0
Order By: Relevance
“…Like in conventional ss-EPI sequences, these artifacts were more commonly found in the SMS-ss-EPI acquisitions than in the rs-EPI acquisitions, which would currently be a major drawback for the use of SMS-ss-EPI in practice. However, recent studies proposed alternative navigator approaches to reduce these artefacts in breast imaging [28],…”
Section: Discussionmentioning
confidence: 99%
“…Like in conventional ss-EPI sequences, these artifacts were more commonly found in the SMS-ss-EPI acquisitions than in the rs-EPI acquisitions, which would currently be a major drawback for the use of SMS-ss-EPI in practice. However, recent studies proposed alternative navigator approaches to reduce these artefacts in breast imaging [28],…”
Section: Discussionmentioning
confidence: 99%
“…In stage 2, residual ghosts were further removed using the reference‐free entropy method 30 . The phase error θ$$ \theta $$ in stage 2 was modeled as a first‐order polynomial 31 : θgoodbreak=πκxfalse/Nxgoodbreak+θ0,$$ \theta =\pi \kappa x/{N}_x+{\theta}_0, $$ where θ0$$ {\theta}_0 $$ = spatially constant phase shift, κ$$ \kappa $$ = phase shift slope (with κ=1$$ \kappa =1 $$ referring to a one‐pixel shift between positive and negative lines), and Nx$$ {N}_x $$ = number of read‐out points. The cost function fentropy()κ,θ0$$ {f}_{entropy}\left(\kappa, {\theta}_0\right) $$ of the image entropy was formulated and minimized to estimate the κ$$ \kappa $$ and θ0$$ {\theta}_0 $$ solutions.…”
Section: Methodsmentioning
confidence: 99%
“…For the acquired SMS‐OLED data, we used a phase search algorithm 45 to reduce the Nyquist ghost artifacts. The acquired data were processed the same as the training samples with MATLAB (Mathworks), and then sent to the trained network for T 2 map reconstruction.…”
Section: Methodsmentioning
confidence: 99%