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Dive into the research topics where Henrik Sandin is active.

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Featured researches published by Henrik Sandin.


Superconductor Science and Technology | 2010

Ultra-low-field MRI for the detection of liquid explosives

Michelle A. Espy; Mark Flynn; John J. Gomez; Christina J. Hanson; Robert H. Kraus; Per E. Magnelind; Karlene Maskaly; Shaun Newman; Tuba Owens; Mark Peters; Henrik Sandin; Igor Savukov; Larry J. Schultz; Algis Urbaitis; Petr L. Volegov; Vadim S. Zotev

Recently it has become both possible and practical to perform MR at magnetic fields from µT to mT, the so-called ultra-low field (ULF) regime. SQUID sensor technology allows for ultra-sensitive detection while pulsed pre-polarizing fields greatly enhance signal. The instrumentation allows for unprecedented flexibility in signal acquisition sequences and simplified MRI instrumentation. Here we present the results for a new application of ULF MRI and relaxometry for the detection and characterization of liquids. We briefly describe the motivation and advantages of the ULF MR approach. We then present recent results from a 7- channel ULF MRI/relaxometer system constructed to non-invasively inspect liquids at a security check-point for the presence of hazardous material. The instrument was fielded to the Albuquerque International Airport in December, 2008, and results from that endeavor are also presented.


IEEE Transactions on Applied Superconductivity | 2007

Multi-Channel SQUID System for MEG and Ultra-Low-Field MRI

Vadim S. Zotev; Andrei N. Matlachov; Petr L. Volegov; Henrik Sandin; Michelle A. Espy; John C. Mosher; Algis Urbaitis; Shaun Newman; Robert H. Kraus

A seven-channel system capable of performing both magnetoencephalography (MEG) and ultra-low-field magnetic resonance imaging (ULF MRI) is described. The system consists of seven second-order SQUID gradiometers with 37 mm diameter and 60 mm baseline, having magnetic field resolution of 1.2-2.8 fT/radicHz . It also includes four sets of coils for 2D Fourier imaging with pre-polarization. The systems MEG performance was demonstrated by measurements of auditory evoked response. The system was also used to obtain a multi-channel 2D image of a whole human hand at the measurement field of 46 microtesla with 3 by 3 mm resolution.


IEEE Transactions on Applied Superconductivity | 2007

Magnetic Sensors for Bioassay: HTS SQUIDs or GMRs?

Chris Carr; Andrei N. Matlachov; Henrik Sandin; Michelle A. Espy; Robert H. Kraus

In this paper we compare the detection of magnetic microparticles by HTS SQUIDs and GMR sensors. Our prototype system uses a HTS SQUID array insulated/isolated from a nonmagnetic tube in which the sample flows at room temperature. This necessarily results in a liftoff between sensor and sample in the range of 2 mm. While HTS SQUIDs typically have an intrinsic noise sensitivity that is at least two orders of magnitude better than conventional GMR sensors (~ 1 pTradicHz for washer SQUIDs compared to ~ 100 pTradicHz for the best commercial GMRs), the dipole like response of a magnetic microparticle in flow is such that this difference in noise performance can be compensated for by the reduction in standoff (order of 0.2 mm) when using a magnetoresistive sensor. Here we detail the two different approaches, present comparative results and discuss the relative merits of each setup.


IEEE Transactions on Applied Superconductivity | 2009

Applications of Ultra-Low Field Magnetic Resonance for Imaging and Materials Studies

Michelle A. Espy; Mark Flynn; John J. Gomez; Christina J. Hanson; Robert H. Kraus; Per E. Magnelind; Karlene Maskaly; Shaun Newman; Mark Peters; Henrik Sandin; Igor Savukov; Larry J. Schultz; Algis Urbaitis; Petr L. Volegov; Vadim S. Zotev

Recently it has become both possible and practical to perform MR at magnetic fields from muT to mT, the so-called ultra-low field (ULF) regime. SQUID sensor technology allows for ultra-sensitive detection while pulsed pre-polarizing fields greatly enhance signal. The instrumentation allows for unprecedented flexibility in signal acquisition sequences. Here we present the results from several applications of ULF MR which exploit the unique abilities of the method. These include novel ways to image both brain structure and function either by combination of MRI with magnetoencephalography or direct observation of the interaction of neural currents with the spin population, and ULF relaxometry for detection and characterization of materials relevant to numerous non-invasive inspection applications. We briefly describe the motivation, advantages, and recent results of several new applications of the ULF MR method. Specifically, we present recent data measuring the interaction of weak ( ~ 10 muA) currents with a spin-population in a water phantom, as studied by ULF MRI with implications for neural current imaging. We also present data from a ULF MR relaxometer developed inspecting liquids in a check-point for the presence of hazardous material.


IEEE Transactions on Applied Superconductivity | 2011

Progress on Detection of Liquid Explosives Using Ultra-Low Field MRI

Michelle A. Espy; Shermiyah Baguisa; David Dunkerley; Per E. Magnelind; Tuba Owens; Henrik Sandin; Igor Savukov; Larry J. Schultz; Algis Urbaitis; Petr L. Volegov

Nuclear magnetic resonance (NMR) spectroscopy and magnetic resonance imaging (MRI) methods are widely used in medicine, chemistry and industry. Over the past several years there has been increasing interest in performing NMR and MRI in the ultra-low field (ULF) regime, with measurement field strengths of 10-100 microTesla and pre-polarization fields of 30-50 mTesla. The real-time signal-to-noise ratio for such measurements is about 100. Our group at LANL has built and demonstrated the performance of SQUID-based ULF NMR/MRI instrumentation for classification of materials and detection of liquid explosives via their relaxation properties measured at ULF, using T1, T2, and T1 frequency dispersion. We are also beginning to investigate the performance of induction coils as sensors. Here we present recent progress on the applications of ULF MR to the detection of liquid explosives, in imaging and relaxometry.


Cytometry Part A | 2006

An instrument for sorting of magnetic microparticles in a magnetic field gradient

Michelle A. Espy; Henrik Sandin; Chris Carr; Christina J. Hanson; Michael D. Ward; Robert H. Kraus

The goal of our bioassay technique is to demonstrate high throughput, highly parallel, and high sensitivity quantitative molecular analysis that will expand current biomedical research capabilities. To this end, we have built and characterized a magnetophoresis instrument using a flow chamber in a magnetic field gradient to sort magnetic microparticles by their magnetic moment for eventual use as biological labels.


Piers Online | 2009

SQUIDs for Magnetic Resonance Imaging at Ultra-low Magnetic Field

Vadim S. Zotev; Robert H. Kraus; Henrik Sandin; Al V. Urbaitis; Petr L. Volegov; Michelle A. Espy

Nuclear magnetic resonance methods are widely used in medicine, chemistry and industry. One application area is magnetic resonance imaging or MRI. It is among the most effective diagnostic tools in medicine. Modern medical MRI scanners use strong magnetic fields. Recently it has become possible to perform NMR and MRI in ultra-low field regime that requires measurement field strengths only of the order of 1 gauss. These ultra-low field techniques exploit the advantages offered by superconducting quantum interference devices or SQUIDs. We describe the world’s first multichannel SQUID-based instruments that are capable of performing ULF MRI for different applications.


IEEE Transactions on Applied Superconductivity | 2015

Progress Toward a Deployable SQUID-Based Ultra-Low Field MRI System for Anatomical Imaging

Michelle A. Espy; Per E. Magnelind; Shaun Newman; Henrik Sandin; Larry J. Schultz; Robert Sedillo; Algis Urbaitis; Petr L. Volegov

Magnetic resonance imaging (MRI) is the best method for non-invasive imaging of soft tissue anatomy, saving countless lives each year. But conventional MRI relies on very high fixed strength magnetic fields, ≥ 1.5 T, with parts-permillion homogeneity, requiring large and expensive magnets. This is because in conventional Faraday-coil based systems the signal scales approximately with the square of the magnetic field. Recent demonstrations have shown that MRI can be performed at much lower magnetic fields (~100 μT, the ULF regime). Through the use of pulsed prepolarization at magnetic fields from ~10-100 mT and SQUID detection during readout (proton Larmor frequencies on the order of a few kHz), some of the signal loss can be mitigated. Our group and others have shown promising applications of ULF MRI of human anatomy including the brain, enhanced contrast between tissues, and imaging in the presence of (and even through) metal. Although much of the required core technology has been demonstrated, ULF MRI systems still suffer from long imaging times, relatively poor quality images, and remain confined to the R&D laboratory due to the strict requirements for a low noise environment isolated from almost all ambient electromagnetic fields. Our goal in the work presented here is to move ULF MRI from a proof-of-concept in our laboratory to a functional prototype that will exploit the inherent advantages of the approach, and enable increased accessibility. Here we present results from a seven-channel SQUID-based system that achieves pre-polarization field of 100 mT over a 200 cm3 volume, is powered with all magnetic field generation from standard MRI amplifier technology, and uses off the shelf data acquisition. As our ultimate aim is unshielded operation, we also demonstrated a seven-channel system that performs ULF MRI outside of heavy magnetically-shielded enclosure. In this paper we present preliminary images and compare them to a model, and characterize the present and expected performance of this system.


Frontiers in Plant Science | 2016

In vivo Observation of Tree Drought Response with Low-Field NMR and Neutron Imaging

Michael W. Malone; Jacob Yoder; James F. Hunter; Michelle A. Espy; Lee T. Dickman; Ron Nelson; Sven C. Vogel; Henrik Sandin; Sanna Sevanto

Using a simple low-field NMR system, we monitored water content in a living tree in a greenhouse over 2 months. By continuously running the system, we observed changes in tree water content on a scale of half an hour. The data showed a diurnal change in water content consistent both with previous NMR and biological observations. Neutron imaging experiments show that our NMR signal is primarily due to water being rapidly transported through the plant, and not to other sources of hydrogen, such as water in cytoplasm, or water in cell walls. After accounting for the role of temperature in the observed NMR signal, we demonstrate a change in the diurnal signal behavior due to simulated drought conditions for the tree. These results illustrate the utility of our system to perform noninvasive measurements of tree water content outside of a temperature controlled environment.


IEEE Transactions on Applied Superconductivity | 2013

Optimization and Configuration of SQUID Sensor Arrays for a MEG-MRI System

E. V. Burmistrov; Henrik Sandin; Larry J. Schultz; Peter Volegov; Michelle A. Espy

The idea of using a large-scale superconducting quantum interference device array for simultaneous detection of both magneto-encephalography (MEG) and magnetic resonance images of the brain at ultra-low field (ULF MRI) is extremely attractive. It could reasonably improve the superposition of images from the two different modalities. Adding a ULF MRI capability to MEG implies the addition of coils for generation of fields and gradients. In addition there is a difference between the optimization criteria for pickup coils. MEG pick-up coils should be small enough to avoid smoothing of spatially sharp field distributions. In the case of ULF MRI the spatial resolution is defined by the applied gradients and the voxel signal-to-noise ratio but not by the pick-up coil diameter. Thus, ULF MRI systems may need fewer pick-up coils of larger size to cover the same area of interest. One approach is a hybrid design with different sizes and quantities of pick-up coils for recording of MEG and MRI signals. We describe a configuration of the 80-channel SQUID array that consists of 64 MEG and 16 MRI magnetometers. We also describe performance of gradiometers in comparison with magnetometers.

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Michelle A. Espy

Los Alamos National Laboratory

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Algis Urbaitis

Los Alamos National Laboratory

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Robert H. Kraus

Los Alamos National Laboratory

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Shaun Newman

Los Alamos National Laboratory

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Larry J. Schultz

Los Alamos National Laboratory

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Igor Savukov

Los Alamos National Laboratory

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Per E. Magnelind

Los Alamos National Laboratory

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Andrei N. Matlachov

Los Alamos National Laboratory

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Vadim S. Zotev

Los Alamos National Laboratory

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