The NMRScopeB plugin into jMRUI is distributed as a component of jMRUI and its use is subject to holding a valid jMRUI license. It is available for free for non-for-profit use and cannot be redistributed or/and modified with the exception for the third party software as stated below. The software shall at no time be used for commercial or industrial purposes without an appropriate license.
Third party software licenses
The computational core of the NMRScopeB 2.0 plug-in has been developed using Python 2.7. Python has an open source license (see Python website).
NMRScopeB uses Java FreeHEP libraries from the FreeHEP VectorGraphics package to which the GNU LGPL license apply. Users are allowed to modify the FreeHEP VectorGraphics package under the GNU LGPL license. For the purpose of debugging these modifications, the users are allowed to use reverse engineering.
Acknowledgement shall be made in all publications resulting from the use of NMRScopeB software. The appropriate reference is currently:
- Z. Starcuk Jr, J. Starcukova, O. Strbak and D. Graveron-Demilly: Simulation of coupled-spin systems in the steady-state free-precession acquisition mode for fast magnetic resonance (MR) spectroscopic imaging. Meas. Sci. Technol. 20, 10, 104033 (2009). DOI: 10.1088/0957-0233/20/10/104033
NMRScopeB is distributed as part of the jMRUI software package, which can be download here. In case of problems or questions contact jana dot starcukova at isibrno dot cz
The NMRScopeB plugin to jMRUI was developed by Zenon Starcuk and Jana Starcukova, at the Institute of Scientific Instruments of the ASCR, v. v. i., Brno, Czech Republic, with the support of grants:
- MRTN-CT-2006-035801, 2006-2010, Advanced Signal Processing for Ultra-Fast Magnetic Resonance Spectroscopic Imaging, and Training, FAST
- PITN-GA-2012-316679, 2012-2017, Transforming Magnetic Resonance Spectroscopy into a Clinical Tool, TRANSACT
- MEYS CR (LO1212) together with EC (ALISI No. CZ.1.05/2.1.00/01.0017), AV0 Z20650511, AVCR (RVO:68081731) and MŠMT CZ.1.05/2.1.00/01.00.