Pre-polarization enhancement by dynamic nuclear polarization in SQUID-based ultra-low-field nuclear magnetic resonance
暂无分享,去创建一个
Yong-Ho Lee | Kiwoong Kim | C. Kang | S. Lee | Yong-Ho Lee | Kiwoong Kim | Chan Seok Kang | Seong-Joo Lee | Seong-min Hwang | Seong-Min Hwang
[1] In-Seon Kim,et al. 64-channel magnetocardiogram system based on double relaxation oscillation SQUID planar gradiometers , 2006 .
[2] Horst Rogalla,et al. (Double) relaxation oscillation SQUIDs with high flux‐to‐voltage transfer: Simulations and experiments , 1994 .
[3] Dietmar Stehlik,et al. Dynamic Nuclear Polarization in Liquids , 1968 .
[4] John S George,et al. Simultaneous magnetoencephalography and SQUID detected nuclear MR in microtesla magnetic fields , 2004, Magnetic resonance in medicine.
[5] I. Rabi,et al. Measurement of Nuclear Spin , 1931 .
[6] H. Hirata,et al. A surface-coil-type resonator for in vivo ESR measurements. , 1994, Journal of magnetic resonance. Series B.
[7] Whittier Myers,et al. Potential Applications of Microtesla Magnetic Resonance ImagingDetected Using a Superconducting Quantum Interference Device , 2006 .
[8] A. Overhauser. Polarization of Nuclei in Metals , 1953 .
[9] H. Swartz,et al. Electronically tunable surface-coil-type resonator for L-band EPR spectroscopy. , 2000, Journal of magnetic resonance.
[10] Robert H Kraus,et al. Microtesla MRI of the human brain combined with MEG. , 2008, Journal of magnetic resonance.
[11] D. Grucker,et al. Dynamic Nuclear Polarization of Water Protons by Saturation of σ and π EPR Transitions of Nitroxides , 1993 .
[12] John Clarke,et al. SQUID-detected magnetic resonance imaging in microtesla fields. , 2007, Annual review of biomedical engineering.
[13] Shingo Matsumoto,et al. Advantageous application of a surface coil to EPR irradiation in overhauser‐enhanced MRI , 2007, Magnetic resonance in medicine.
[14] Hyukchan Kwon,et al. Double Relaxation Oscillation SQUID with High Flux-to-Voltage Transfer and its Application to a Biomagnetic Multichannel System , 1998 .
[15] Low-field EPR measurements by field-cycled dynamic nuclear polarization , 1991 .
[16] Gen Uehara,et al. High sensitivity double relaxation oscillation superconducting quantum interference devices with large transfer from flux to voltage , 1995 .
[17] F. Robb,et al. The Application of Proton-Electron Double-Resonance Imaging Techniques to Proton Mobility Studies , 1994 .
[18] Brandon D. Armstrong,et al. Hyperpolarized water as an authentic magnetic resonance imaging contrast agent , 2007, Proceedings of the National Academy of Sciences.
[19] Martin Burghoff,et al. Nuclear magnetic resonance in the nanoTesla range , 2005 .
[20] Yon-Kyu Park,et al. Double relaxation oscillation SQUID with reference junction for biomagnetic multichannel applications , 1997 .
[21] Heisenberg spin exchange effects of nitroxide radicals on Overhauser dynamic nuclear polarization in the low field limit at 1.5mT. , 2010, Journal of magnetic resonance.
[22] Robert McDermott,et al. Liquid-State NMR and Scalar Couplings in Microtesla Magnetic Fields , 2002, Science.
[23] Jaap Flokstra,et al. Second generation dc-SQUID sensors: relaxation oscillation SQUIDS (ROS) with frequency readout and double relaxation oscillation SQUIDS (DROS) with voltage readout , 1994, Photonics West - Lasers and Applications in Science and Engineering.