Ultra-low Field Nuclear Magnetic Resonance Measurements with SQUIDs

Slides:



Advertisements
Similar presentations
Richard Wise FMRI Director +44(0)
Advertisements

PHYSICS OF MAGNETIC RESONANCE
MR TRACKING METHODS Dr. Dan Gamliel, Dept. of Medical Physics,
SQUID NMR Measurements in nEDM experiment -- how to get a big signal & how to operate SQUIDs in High Voltage Environments Chen-Yu Liu.
The Basics of MRI The Basics of MRI. Current MRI technology displays images as multiple sets of gray tone images. Visualization and interpretation of.
MRI “Magnetic Resonance Imaging”. Nuclei with nuclear spin: elementary magnets Magnetic moment:  =magnetogyric ratio L=angular momentum.
Nuclear Magnetic Resonance
NMR Spectroscopy Tuning / Matching Shimming and Lock.
NMR Nuclear Magnetic Resonance Spectroscopy. Over the past fifty years nuclear magnetic resonance spectroscopy, commonly referred to as nmr, has become.
MRI. Magnetic Resonance 1.Principle first observed in Used for spectroscopy and imaging 3.Imaging techniques are a form of tomography, where slices.
NMR SPECTROSCOPY.
ELEG 479 Lecture #9 Magnetic Resonance (MR) Imaging
NMR Nuclear Magnetic Resonance. 1 H, 13 C, 15 N, 19 F, 31 P.
Faraday’s Law  produces an induced current Lenz’s Law: Induced current is in a direction so as to produce a B opposing the change in magnetic flux, 
Structure Determination by NMR CHY 431 Biological Chemistry Karl D. Bishop, Ph.D. Lecture 1 - Introduction to NMR Lecture 2 - 2D NMR, resonance assignments.
NMR Spectroscopy Part II. Signals of NMR. Free Induction Decay (FID) FID represents the time-domain response of the spin system following application.
Nuclear Magnetic Resonance Spectrometry Chap 19
Spectroscopy 3: Magnetic Resonance CHAPTER 15. Pulse Techniques in NMR The “new technique” Rather than search for and detect each individual resonance,
Resonance condition. Pulse A coil of wire placed around the X axis will provide a magnetic field along the X axis when a direct current is passed through.
Basics Concepts Nuclear spins Magnetic field B 0 Energy Sensitivity The NMR transition Larmor Frequency Magnetic field B 1 The rotating frame A pulse!
Magnetic Resonance MSN 506 Notes. Overview Essential magnetic resonance Measurement of magnetic resonance Spectroscopic information obtained by magnetic.
MRI: an Introduction By Mohammad Ali Ahmadi Pajouh Amirkabir University of Technology Biomedical Eng. Dep.
Medical Imaging Systems: MRI Image Formation
ELEG 479 Lecture #12 Magnetic Resonance (MR) Imaging
Detection of 3He with SQUIDs. Experimental parameters For B=300 Gauss The expected signal is 220 fT (specific geometry is taken into account), while the.
Magnetic Resonance Imaging
CT “Computer tomography”. Contrast mechanisms in X-ray imaging: X-ray absorption X-ray absorption mechanisms: 1. Photoelectric effect 2. Compton scatter.
Seminar October, 2008 j. brnjas-kraljević. Imaging (MRI)  tomography technique  tomography technique – the volume image is built up by images of thin.
Medical Imaging Systems: MRI Image Formation
Electromagnetic shielding of the SQUID in the nEDM Experiment: Bolts and Nuts Andrei Matlashov, Michelle Espy, LANL, P What happens when SQUID is.
Nuclear Magnetic Resonance ANIMATED ILLUSTRATIONS MS Powerpoint Presentation Files Uses Animation Schemes as available in MS XP or MS 2003 versions A class.
September, 2003BME 1450 Introduction to NMR 1 Nuclear Magnetic Resonance (NMR) is a phenomenon discovered about 60 years ago.
NMR in Medicine and Biology
Michelle Espy SQUID NMR Signal Outline Overview of SQUIDs in EDM: present thinking - experimental design ideas - expected signal,
Human Functional Brain Imaging Dr. Ryan C.N. D’Arcy NRC Institute for Biodiagnostics (Atlantic)
1 Introduction to Biomolecular NMR. 2 Nuclear Magnetic Resonance Spectroscopy Certain isotopes ( 1 H, 13 C, 15 N, 31 P ) have intrinsic magnetic moment.
Pei-Ann Lin and PJ Velez December 13, 2011
3 He Polarization Tests at UIUC Danielle Chandler David Howell UIUC.
SQUID Performance in a HV Environment
Low–field NMR (or MRI) Images of Laser polarized Noble Gas.
Low Field Nuclear Magnetic Resonance High Field (Resolution) NMR: 7.5 T < B < 37 T Study of chemical structures, reactions (only solution) Low Field (Resolution)
Protons (hydrogen nuclei act like little magnets) MRI Collective Magnetic Moment of Protons (M 0 ) Each pixel is a glass of protons B 0 = 3T (not to scale)
Biomolecular Nuclear Magnetic Resonance Spectroscopy BASIC CONCEPTS OF NMR How does NMR work? Pulse FT NMR 2D NMR experiments nD NMR experiments 01/15/03.
PULSED NMRAcquire F.I.D. Free Induction Decay NMR detection soon after a strong pulse: precessing nuclear magnetization induces a signal in coil when it.
Study of T 1 relaxation time A proposal to test T 1 using a dilution fridge and SQUID NMA at Royal Hollow University,London.
NMR Nuclear Magnetic Resonance Chapter 13. Proton Nuclear Spin States Two states have the same energy in the absence of a magnetic field Magnetic Field.
Lecture 1: Magnetic Resonance
Real time shimming (RTS) for compensation of respiratory induced field changes P van Gelderen, JA de Zwart, P Starewicz, RS Hinks, JH Duyn Introduction.
Biomolecular Nuclear Magnetic Resonance Spectroscopy
Melanie Martin University of Winnipeg
Nuclear Magnetic Resonance Spectroscopy
(Instrument part) Thanundon Kongnok M
Imaging Science Department, IC Jo Hajnal
Biophysical Tools '04 - NMR part II
Spatial Encoding: Sub mm from meter sized RF
An Optimal Design Method for MRI Teardrop Gradient Waveforms
MRI Pulse Sequences: IR, EPI, PC, 2D and 3D
Magnetic Susceptibility
Introduction to diffusion MRI
Basic MRI I Chapter 3 Notes.
10.5 Fourier Transform NMR Instrumentation
10.6 Fourier Transform Mass Spectrometry
MEG fundamentals.
CHY 431 Biological Chemistry
Structure determination by NMR
Introduction to diffusion MRI
1H and 13C NMR Spectroscopy in Organic Chemistry
Fig. 2 Characterization of prepolarized NV NMR.
(4)ELECTRONIC SUPPORT SYSTEM
Presentation transcript:

Ultra-low Field Nuclear Magnetic Resonance Measurements with SQUIDs Michelle Espy SQUID Team Biological and Quantum Physics, P-21

A SQUID is a magnetic flux to voltage converter

Magnetometers and Gradiometers

T < 0.5 K can be a problem for SQUIDs The low temperature is required to keep the 3He diffusion coefficient sufficiently high. The white component of SQUID noise energy is proportional to temperature. But the same is not necessarily true for the 1/f component. Most SQUIDs are optimized for operation at 4 K.

Use the SQUIDs to measure 3 and get rid of your dependence on B Any difference in for Eparallel or Eantiparallel is your signal for an EDM Use the SQUIDs to measure 3 and get rid of your dependence on B

Introduction to Ultra-Low Field NMR By ULF we mean measurement fields from 1 – 100 mT EDM ~0.3 mT Separate polarizing and measurement fields (B0 vs Bm ) Dramatically smaller and lower-cost systems Narrow line widths (wFWHM a B0 or Bm) Reduced susceptibility ‘artifact’ (a B0 or Bm) Compatible with MEG (simultaneous MEG/MRI) Potential to directly measure neuronal currents Micro MRI possible

Ultra Low Field NMR This decaying NMR signal is called the Free Induction Decay, or FID.  The actual spectrum is recovered from the FID via Fourier transformation, which transforms the time interferogram into a frequency spectrum. The signal frequency, w0 = gB0 (Larmor frequency) scales with B0.

Line width for frog (not anesthetized) ~ 2 Hz First ultra-low-field NMR for living animal Line width for frog (not anesthetized) ~ 2 Hz B0 = 60 G, Bm = 47 µT

G 1-D gradient image of a water phantom at 50 mT 1-volume and 3-section water phantoms: G Feasibility of imaging demonstrated by these data!

2-D gradient image of a water phantom at 50 mT

First-ever simultaneous NMR-MEG recording Simultaneous MEG ultra-low-field NMR measurements: B0 = 60 G, Bm ~ 5.5 mT

Jena Gradiometer Planar gradiometer with 2 cm x 2 cm coils connected in series Baseline is 4 cm. Effective area of 7.1 mm2 (one loop). The measured white noise level 5 – 10 mF/sqrt(Hz) Magnetic field gradient resolution 36 – 72 fT m-1 Hz-1/2 Corresponds to a field resolution in one gradiometer loop from 1.45 – 2.9 fT Hz-1/2. Measurements in a uniform field showed a balance from 104 m-1 to 103 m-1.

How does our water signal compare to what we expect? At 1 mT and 298K

We have developed electronics such that the SQUID survives the pulsed fields Dead time after SQUID reset: SQUID/electronics to recover = 20 ms Bp to SQUID = 5-10 ms (best 1.5 ms)

UIUC apparatus

SQUID gradiometer

Simultaneous dressed spin – will SQUID survive? Proposed dressed spin field ~ 1 mT at 1 kHz SQUID sensitivity is 1 nT/F - for 1000 F/s That is a high slew rate for SQUID (though not impossible) Use of a gradiometer would solve the problem Balance level 103 for Jena gradiometer Reduce signal to 1 F/s Expected signal at ~ 3 Hz – so other filtering methods can also be used