SQUIDs - Low Temperature Laboratory

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Microtesla Nuclear Magnetic Resonance and Magnetic Resonance Imaging • Nuclear magnetic resonance • Magnetic resonance imaging Michael Hatridge Nathan Kelso SeungKyun Lee Robert McDermott Michael Mössle Michael Mück Whit Myers Bennie ten Haken Andreas Trabesinger Erwin Hahn Alex Pines
Energy z B 0 Nuclear Magnetic Resonance Protons M B 0 E = +µ p B ν 0 = 42.58 MHz/tesla ω0 = γB0 E = -µ pB Magnetic moment (µpB0
Page 1 and 2: SQUIDs: From Cosmology to Magnetic
Page 3 and 4: Milestones in Superconductivity 191
Page 5 and 6: The Discovery of Superconductivity
Page 7 and 8: Zero Resistance Magnetic field •
Page 13 and 14: Flux Quantization Φ = n Φ 0 J Φ
Page 15 and 16: • Cooper pairs tunnel through bar
Page 17 and 18: Temperature (Kelvin) Transition Tem
Page 21 and 22: The dc Superconducting Quantum Inte
Page 23 and 24: B N ~ 1 fT Hz -1/2 Superconducting
Page 25 and 26: Applications of SQUIDs: An Overview
Page 27 and 28: Neuromag ® 306-Channel SQUID Syste
Page 29 and 30: CardioMag Imaging System for Magnet
Page 31 and 32: 2G Superconducting Rock Magnetomete
Page 33 and 34: MAGMA-C1 Scanning SQUID Microscope
Page 35 and 36: Courtesy Stanford University and NA
Page 37 and 38: Searching for Axions: The Microstri
Page 39 and 40: Resonant Conversion of Axions into
Page 41 and 42: Noise Temperature R T -A [ T + T (
Page 43 and 44: Microstrip SQUID Amplifier Conventi
Page 45 and 46: Noise Temperature of Microstrip Amp
Page 47: Summary • Gain ≥ 20 dB for freq
Page 52 and 53: Timeline Michael Crichton, 1999 “
Page 57 and 58: Three dimensional images of pepper
Page 59: B = 13.2 mT int T 1 contrast images
Page 62: Future directions for low-field MRI

SQUIDs - Low Temperature Laboratory

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