@article{MonteliusLjungbergHornetal.2012,
  author    = {Montelius, Mikael and Ljungberg, Maria and Horn, Michael and Forssell-Aronsson, Eva},
  title     = {Tumour size measurement in a mouse model using high resolution MRI},
  series = {BMC Medical Imaging},
  volume    = {12},
  journal   = {BMC Medical Imaging},
  number    = {12},
  doi       = {10.1186/1471-2342-12-12},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-124049},
  year      = {2012},
  abstract  = {Background Animal models are frequently used to assess new treatment methods in cancer research. MRI offers a non-invasive in vivo monitoring of tumour tissue and thus allows longitudinal measurements of treatment effects, without the need for large cohorts of animals. Tumour size is an important biomarker of the disease development, but to our knowledge, MRI based size measurements have not yet been verified for small tumours (10-2-10-1 g). The aim of this study was to assess the accuracy of MRI based tumour size measurements of small tumours on mice. Methods 2D and 3D T2-weighted RARE images of tumour bearing mice were acquired in vivo using a 7 T dedicated animal MR system. For the 3D images the acquired image resolution was varied. The images were exported to a PC workstation where the tumour mass was determined assuming a density of 1 g/cm3, using an in-house developed tool for segmentation and delineation. The resulting data were compared to the weight of the resected tumours after sacrifice of the animal using regression analysis. Results Strong correlations were demonstrated between MRI- and necropsy determined masses. In general, 3D acquisition was not a prerequisite for high accuracy. However, it was slightly more accurate than 2D when small (<0.2 g) tumours were assessed for inter- and intraobserver variation. In 3D images, the voxel sizes could be increased from 1603 μm3 to 2403 μm3 without affecting the results significantly, thus reducing acquisition time substantially. Conclusions 2D MRI was sufficient for accurate tumour size measurement, except for small tumours (<0.2 g) where 3D acquisition was necessary to reduce interobserver variation. Acquisition times between 15 and 50 minutes, depending on tumour size, were sufficient for accurate tumour volume measurement. Hence, it is possible to include further MR investigations of the tumour, such as tissue perfusion, diffusion or metabolic composition in the same MR session.},
  language  = {en}
}
@article{NordbeckBeerKoestleretal.2012,
  author    = {Nordbeck, Peter and Beer, Meinrad and K{\"o}stler, Herbert and Ladd, Mark E. and Quick, Harald H. and Bauer, Wolfgang R. and Ritter, Oliver},
  title     = {Cardiac catheter ablation under real-time magnetic resonance guidance},
  series = {European Heart Journal},
  volume    = {33},
  journal   = {European Heart Journal},
  number    = {15},
  doi       = {10.1093/eurheartj/ehs139},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-125638},
  year      = {2012},
  abstract  = {One of the main shortcomings of interventional electrophysiology (EP) is its inability to generate sufficient soft tissue contrast for intra-procedural visualization of the myocardium and the surrounding tissue, using conventional imaging techniques. Interventional cardiovascular magnetic resonance imaging (MRI) aims at bringing about significant improvements to the complex and decisive EP interventions far beyond the capabilities of currently available supportive imaging techniques used to surmount the drawbacks of fluoroscopy, as MRI not only allows of precise three-dimensional exposure of the cardiovascular morphology, but also proves to be a promising technique exclusively suitable for direct visualization of arrhythmogenic substrate and therapeutic effects. The major challenge posed by clinical …},
  language  = {en}
}
@phdthesis{Purea2008,
  author    = {Purea, Edmund Armin},
  title     = {New Methods and Applications in Nuclear Magnetic Resonance Microscopy using small RF Coils},
  url       = {http://nbn-resolving.de/urn:nbn:de:bvb:20-opus-31066},
  school      = {Universit{\"a}t W{\"u}rzburg},
  year      = {2008},
  abstract  = {Nuclear magnetic resonance (NMR) imaging is a well-established imaging technique. If the achieved spatial resolution is below 100 um, it is usually denoted as magnetic resonance microscopy (MRM). The spatial resolution limit is on the order of a few um. As a downside, high resolution imaging is usually time-consuming and technological requirements are very sumptuous. Furthermore, miniaturization of the radiofrequency (RF) coil leading to a so-called microcoil is necessary; it also brings along detrimental effects. Therefore, there is a high potential for optimizing present MRM methods. Hence it is the aim of this work to improve and further develop present methods in MRM with focus on the RF coil and to apply those methods on new biological applications. All experiments were conducted on a Bruker 17.6 T system with a maximum gradient strength of 1 T/m and four RF receiver channels. Minimizing the RF coil dimensions, leads to increased artefacts due to differences in magnetic susceptibility of the coil wire and surrounding air. Susceptibility matching by immersing the coil in FC-43 is the most common approach that fulfills the requirements of most applications. However, hardly any alternatives are known for cases where usage of FC-43 is not feasible due to its specific disadvantages. Two alternative substances (bromotricholoromethane and Fomblin Y25) were presented and their usability was checked by susceptibility determination and demonstration experiments after shimming under practical conditions. In a typical MRM microcoil experiment, the sample volume is significantly smaller than the maximum volume usable for imaging. This mismatch has been optimized in order to increase the experiment efficiency by increasing the number of probe coils and samples used. A four-channel probehead consisting of four individual solenoid coils suited for cellular imaging of Xenopus laevis oocytes was designed, allowing simultaneous acquisition from four samples. All coils were well isolated and allowed quantitative image acquisition with the same spatial resolution as in single coil operation. This method has also been applied in other studies for increased efficiency: using X. laevis oocytes as a single cell model, the effect of chemical fixation on intracellular NMR relaxation times T1 and T2 and on diffusion was studied for the first time. Significant reduction of relaxation times was found in all cell compartments; after reimmersion in buffer, values return close to the initial values, but there were small but statistically significant differences due to residual formaldehyde. Embryos of the same species have been studied morphologically in different developmental stages. Wild type embryos were compared to embryos that had experienced variations in protein levels of chromosomal proteins HMGN and H1A. Significant differences were found between wild type and HMGN-modified embryos, while no difference was observed between wild type and H1-modified embryos. These results were concordant with results obtained from light microscopy and histology. The technique of molecular imaging was also performed on X. laevis embryos. Commercially available antibodies coupled to ultrasmall superparamagnetic iron oxide (USPIO) dextrane coated particles (MACS) served as a specific probe detectable by MRM, the aim being the detection of tissue specific contrast variations. Initially, the relaxivity of MACS was studied and compared to Resovist and VSOP particles. The iron concentration was determined quantitatively by using a general theoretical approach and results were compared to values obtained from mass spectroscopy. After incubation with MACS antibodies, intraembryonal relaxation times were determined in different regions of the embryo. These values allowed determination of local iron oxide particle concentrations, and specific binding could be distinguished from unspecific binding. Although applications in this work were focused on X. laevis oocytes and embryos, 3D-imaging on a beewolf head was also carried out in order to visualize the postpharyngeal gland. Additionally, an isolated beewolf antenna was imaged with a spatial resolution of (8 um)^3 for depiction of the antennal glands by using a microcoil that was specially designed for this sample. The experiments carried out in this work show that commercially available MRM systems can be significantly optimized by using small sample-adapted RF coils and by parallel operation of multiple coils, by which the sample throughput and thus time-efficiency is increased. With this optimized setup, practical use was demonstrated in a number of new biological applications.},
  subject      = {Magnetische Resonanz},
  language  = {en}
}