Imaging tumor hypoxia by magnetic resonance methods

Authors

  • Jesús Pacheco-Torres,

    1. Laboratory for Imaging and Spectroscopy by Magnetic Resonance LISMAR, Institute of Biomedical Research Alberto Sols, CSIC/UAM, c/ Arturo Duperier 4, Madrid, Spain
    2. Laboratory of Organic Synthesis and Molecular Imaging by Magnetic Resonance, School of Chemistry, University at a Distance, P° Senda del Rey 9, Madrid 28040, Spain
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  • Pilar López-Larrubia,

    1. Laboratory for Imaging and Spectroscopy by Magnetic Resonance LISMAR, Institute of Biomedical Research Alberto Sols, CSIC/UAM, c/ Arturo Duperier 4, Madrid, Spain
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  • Paloma Ballesteros,

    1. Laboratory of Organic Synthesis and Molecular Imaging by Magnetic Resonance, School of Chemistry, University at a Distance, P° Senda del Rey 9, Madrid 28040, Spain
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  • Sebastián Cerdán

    Corresponding author
    1. Laboratory for Imaging and Spectroscopy by Magnetic Resonance LISMAR, Institute of Biomedical Research Alberto Sols, CSIC/UAM, c/ Arturo Duperier 4, Madrid, Spain
    • Instituto de Investigaciones Biomédicas ‘Alberto Sols’, c/Arturo Duperier 4, Madrid 28029, Spain.
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Abstract

Tumor hypoxia results from the negative balance between the oxygen demands of the tissue and the capacity of the neovasculature to deliver sufficient oxygen. The resulting oxygen deficit has important consequences with regard to the aggressiveness and malignancy of tumors, as well as their resistance to therapy, endowing the imaging of hypoxia with vital repercussions in tumor prognosis and therapy design. The molecular and cellular events underlying hypoxia are mediated mainly through hypoxia-inducible factor, a transcription factor with pleiotropic effects over a variety of cellular processes, including oncologic transformation, invasion and metastasis. However, few methodologies have been able to monitor noninvasively the oxygen tensions in vivo. MRI and MRS are often used for this purpose. Most MRI approaches are based on the effects of the local oxygen tension on: (i) the relaxation times of 19F or 1H indicators, such as perfluorocarbons or their 1H analogs; (ii) the hemodynamics and magnetic susceptibility effects of oxy- and deoxyhemoglobin; and (iii) the effects of paramagnetic oxygen on the relaxation times of tissue water. 19F MRS approaches monitor tumor hypoxia through the selective accumulation of reduced nitroimidazole derivatives in hypoxic zones, whereas electron spin resonance methods determine the oxygen level through its influence on the linewidths of appropriate paramagnetic probes in vivo. Finally, Overhauser-enhanced MRI combines the sensitivity of EPR methodology with the resolution of MRI, providing a window into the future use of hyperpolarized oxygen probes. Copyright © 2010 John Wiley & Sons, Ltd.

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