% IMPORTANT: The following is UTF-8 encoded.  This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.

@ARTICLE{Wang:306610,
      author       = {Y. Wang$^*$ and M. W. May and M. Gratz and M. Ladd$^*$ and
                      S. Orzada$^*$},
      title        = {{U}ltimate {I}ntrinsic {SNR} in the {T}orso of {R}ealistic
                      {B}ody {M}odels.},
      journal      = {Magnetic resonance in medicine},
      volume       = {95},
      number       = {4},
      issn         = {1522-2594},
      address      = {New York, NY [u.a.]},
      publisher    = {Wiley-Liss},
      reportid     = {DKFZ-2025-02647},
      pages        = {2409-2419},
      year         = {2026},
      note         = {#EA:E020#LA:E020# / 2026 Apr;95(4):2409-2419},
      abstract     = {This work aims to investigate how the ultimate intrinsic
                      signal-to-noise ratio (uiSNR) varies with increasing static
                      magnetic field B 0 $$ {B}_0 $$ in the torso of realistic
                      body models.A dipole cloud was positioned around the
                      realistic body model and randomly excited. The volume
                      integral solver MARIE was used to calculate the
                      corresponding electromagnetic fields. The uiSNR maps were
                      calculated using these electromagnetic bases and were fitted
                      with the power law for different B 0 $$ {B}_0 $$ ranges.The
                      uiSNR could be reliably calculated in regions deeper than 3
                      cm, where convergence of uiSNR over the number of basis
                      vectors was achieved. In a lower magnetic field range (from
                      0.55 to 3 T), the uiSNR increases roughly linearly versus B
                      0 $$ {B}_0 $$ with small variation throughout the torso
                      (Ella: uiSNR ∝ B0 0.96±0.07, Duke: uiSNR ∝ B0
                      0.98±0.10). In an upper magnetic field range (from 5 to 14
                      T), the uiSNR increases superlinearly in the torso (Ella:
                      uiSNR ∝ B0 1.86±0.25, Duke: uiSNR ∝ B0 1.99±0.28),
                      with a larger variation correlated to the heterogeneous
                      structure of the body model.The superlinear scaling exponent
                      in the upper magnetic field range indicates the promise of
                      applying UHF MRI for body imaging.},
      keywords     = {MRI (Other) / in silico (Other) / torso (Other) / uiSNR
                      (Other)},
      cin          = {E020},
      ddc          = {610},
      cid          = {I:(DE-He78)E020-20160331},
      pnm          = {315 - Bildgebung und Radioonkologie (POF4-315)},
      pid          = {G:(DE-HGF)POF4-315},
      typ          = {PUB:(DE-HGF)16},
      pubmed       = {pmid:41299668},
      doi          = {10.1002/mrm.70202},
      url          = {https://inrepo02.dkfz.de/record/306610},
}