WHITE PAPER ON BRAIN DISORDER PHENOMENOLOGY USING NONINVASIVE BRAIN ANALYSIS
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White Paper on
Brain Disorder Phenomenology Using
Noninvasive Brain Analysis
Presented by
Sandia National Laboratories
P. O. Box 5800
Low Observable Projects Department
Department 9735
Albuquerque, NM 87185-5800
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1. Executive Summary
A. Proposed Work
We propose the formation of a scientific center of excellence for the purpose of developing and
evaluating superconducting instrumentation and high fidelity computational electromagnetic brain
models for the high resolution study of human brain activity. The proposed center will utilize the
strengths and expertise of scientists in New Mexico, including physicists, engineers, and medical
neuroscientists. Working together, this team will translate their knowledge in diverse areas such
as superconductivity, cryogenics, electronics, image processing, computational electromagnetics,
advanced signal analysis, and neuroscience to develop hardware, software, analyses, and medical
applications for a new generation of brain imaging systems. Such imaging systems would consist
of a 1000 sensor biomagnetometer, parallel supercomputer, and graphic workstation operating
seamlessly to translate the brain's magnetic and electrical signals into a three-dimensional moving
image showing it's instantaneous intensity and distribution. This instrument, coupled with
advanced signal processing techniques and a computational electromagnetic brain model, will be
used to study the brain in health and disease states. The knowledge gained in medical and basic
science about the brain could be used to:
1. Lower Health Care Costs: Health care costs for neurological disorders can be reduced
through the development and use of more specific and sensitive diagnostics.
2. Minimize Surgical Risks: The risk to critical areas of the brain may be reduced by
identifying those areas noninvasively, and sparing them during neurosurgery.
3. New and Improved Treatments: We can improve the treatment of neurological
diseases by using tomographic images of the brain's activity to provide immediate
quantitative feedback of how the brain responds to that treatment.
4. Psychiatric Disorders: The proposed noninvasive brain imaging system and
computational model will expand our understanding and treatment of mental illnesses.
5. Basic Neuroscience: The proposed center, instrumentation, and computational model
will further our knowledge of the higher functions of the brain--the essence of what it is to
be human.
The research instrumentation and computational electromagnetic brain model will be offered as a
national resource center for the study of the brain. The technology developed for this
biomagnetometer will be made available to U. S. industries, expanding our competitiveness in the
international medical instrumentation marketplace.
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B. Technical Benefits
In order to develop an advanced neuromagnetometer, we will need to develop technology in the
following areas:
1. Superconducting sensors: Thin-film SQUID (Superconducting Quantum Interference
Device) magnetic sensors will be designed to improve upon the sensitivity and dynamic
range of existing designs. An all digital sensor design will reduce parts count that will
improve manufacturability and enable us to expand the number of sensors without
increasing complexity. SQUID sensor development has extended application in many
areas of remote sensing, where the highest attainable sensitivity is of importance.
2. Cryocoolers and Cryostats: Cryocoolers and low loss cryostats will be developed so
as to reduce the size and portability, while increasing the flexibility of existing dewars.
Instead of relying on a large reservoir of liquid helium for cooling, we propose developing
low temperature, high efficiency, long-life refrigeration systems, thus reducing the 1000
sensor array to a "hair dryer" enclosure. The cryocooler technology we will develop will
also benefit other types of low-noise sensors and portable quantum standards.
3. Image processing: We will develop computer algorithms for three dimensional
segmentation of medical images from CT or MRI scans. Specifically, processes will be
developed and tested to automatically recognize the different tissue types in the brain--
scalp, skull, dura, cortex, blood vessels, etc.--and create a model of each surface, layer by
layer. This model will be used for electromagnetic calculations of the magnetic fields and
electrical potentials resulting from brain activity.. Automated image segmentation will also
be valuable to radiologists, in that portions of the brain (as well as other organs) will be
more readily visualized without the intervening tissue layers--i.e., as they might appear
during surgery.
4. Computational electromagnetics: The segmented model of the various tissues in the
head, known as a finite element model (FEM), will be used to provide a high accuracy
prediction of the magnetic fields and electrical potentials resulting from the brain's
electrical activity. This is called the forward solution. A highly accurate forward solution
is necessary in order to compute a high resolution unambiguous estimate of the brain's
activity. Because of the complexity of these calculations, software will be developed for
high speed parallel computer systems.
5. Signal processing: What does one do with 1000 channels of brain signal information?
The classical EEG notion of displaying each individual channel on a chart recorder is both
impractical and wasteful of the rich information of such a large array. Instead, we propose
deriving signal processing techniques from the array processing used in phased array
radar. This would enable the array of 1000 sensors to be instantaneously "steered" to any
part of the brain, receiving the brain's signals with much higher sensitivity and selectivity
than any single sensor. The array could then be "scanned" through the three-dimensional
volume of the brain, generating a tomographic picture of its activity. This type of signal
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processing would also improve the array's rejection of magnetic disturbances, such that an
expensive and bulky magnetically shielded room will no longer be required for
neuromagnetic measurements.
C. Recommendations
The proposed project utilizes scientific and engineering expertise that is unique to New Mexico.
Success in any single portion of this project can boost our technological competitiveness in the
world marketplace. The 90's have been dubbed, "The Decade of the Brain." This work will
advance a noninvasive technology from a laboratory curiosity to commercially viable
instrumentation, lending that phrase new meaning. In three years, New Mexico will host an
international meeting on biomagnetism. The proposed center will demonstrate our creativity and
know-how to the world scientific community. This project has low risk and a large potential
benefit to medicine and neuroscience. We therefore strongly recommend its approval.
D. Scientific and Engineering Research Partners
The scientific and engineering research partners for this effort consists of components from each
of the following areas: Government, National Laboratories, Industry, and Academia.
Sandia National Laboratories brings experience in massively parallel supercomputer applications,
cryogenic support systems, finite element modeling, and computational electromagnetics.
Veterans Administration/Center for Magnetoencephalagraphy brings experience in neurological
phemeneurology, medical imaging, and has experimentation facilities.
The industrial partners would consist of IBM, TRW, and Conductus for SQUID design and
fabrication alternatives.
The Academic partners consists of University of New Mexico, University of Houston, and the
University of Arizona who collectively bring expertise in signal/image processing, finite element
modeling for biological applications, radiological imaging, and neurology.
II. Introduction
In todays society brain disorders devastate the lives of 20% of the total population or
approximately 50 million people. In monetary terms the per capita cost is $1690, which equates
to approximately $400 billion per year or 7.3% of the Gross Domestic Product. This figure
includes both direct costs such as medical treatement and services, and indirect costs such as lost
wages and family caregiving expenses. In proportion the direct costs equal approximately one-
fourth to one-half of the total ($104 billion in 1991) while the indirect costs make up the rest
($296 billion in 1991).
Brain disorders include well over 650 disorders that can be divided into three general categories.
Psychiatric disease ranging from schizophrenia to cognitive impairment account for of $136
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billion in costs. Neurologic disorders - dementia, mental retardation, multiple sclerosis, head and
spinal cord injuries, stroke, cerebral palsy, and epilepsy - cost $103 billion. Disorders of addiction
such as alcohol and drug abuse cost $161 billion. Some disorders such as multiple scleroses are
killers and as a category, brain disorders are a leading cause of death in the United States today.
They are the most common and severe cause of social, economic, and psychological disabilities in
this country.
Empirical medicine has played a centrol role in understanding brain disorders. Much of the
current medical knowledge relating to understanding brain function has relied heavily upon
experiments conducted on surviving victims of unfortunate experiments of nature, such as stroke.
In fact, most of what is currently known about the localization of normal language comes from
the study of aphasia, a disorder of language that is found most often in patients who have suffered
from a stroke or head trauma. Furthermore, almost everything we know about the anatomical
organization of language and memory comes from clinical studies of patients with lesions of the
brain. Today correlation of major mental illnesses to normal and abnormal brain activity is based
primarily on postmortem studies, animal research, and the examination of peripheral metabolites
in human beings. Ultimately one would like to somehow map the vast range of cognitive
functions that become distorted or diminished, leading to brain disorders, by observing the
structure and metabolic and neurochemical function of the brains of normal individuals.
Serious brain disorders including anatomical and functional disorders typically possess
characteristically abnormal electrical signatures that can be directly determined or inferred through
current measurement techniques. The current technology used in diagnosing such disorders are
categorized below with relevant examples of each technology.
1. Active - Invasive: This category is characterized by requiring either direct access to
the brain for stimulation or injection of radioactive sources that can be tracked by
detectors.
Position - emission tomography (PET) is a nonsurgical technique that falls within this
category. It provides images of brain function and has revolutionized the study of human
cognitive processes and psychiatric and neurological disease. This emission tomography
technique requires one to substitute position - emitting isotopes (half-lives ranging from
several minutes to several hours) for constituents of biologically important compounds
such as oxygen, carbon, nitrogen, and hydrogen. The specific isotope is then injected or
inhaled by the patient and subsequently accumulates in specific regions of the brain
according to metabolic activity. In the process of position emission the isotope produces
two gamma rays that can be detected and used for imaging concentrations of the isotope
within the brain. Thereby localizing brain metabolic activity that must have electrical
counterparts. Because PET scanning relies on radiopharmaceuticals, it is unsuitable for
routine testing or therapeutic monitoring.
II. Active - Noninvasive: This category is characterized by requiring either the use of
energetic radiation or stimulated emission by constituent atomic nuclei.
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X-ray computerized tomography (CT) allows one to explore the regional anatomy of the
brain in normal subjects and in patients suffering from neurological disease. Developed in
the early 1970's, CT is the oldest brain imaging technique. In contrast to conventional
radiography, the CT scan distinguishes gray and white matter. It provides images of bone,
brain tissue, and cerebrospinal fluid. Even structures within the brain can be distinguished.
Because it reveals anatomical detail, computerized tomography has greatly expanded the
clinician's capacity for diagnosis. Nevertheless, the views of the brain produced by CT are
static, i.e., CT scans allow one to explore the structure but not the function of the brain.
To produce images of the dynamics of the living brain, other techniques must be combined
with CT.
Magnetic resonance imaging (MRI) is based on computerized tomography and has been
used to explore brain function as well as structure. It is a powerful imaging technique that
can distinguish different body tissues because of their individual chemical composition.
MRI requires a subject to be exposed to a pulsed radio frequency signal superimposed on
a strong magnetic field gradient. The pulsed field stimulates the atomic nuclei to emit
radio waves at characteristic frequencies dependent on the nuclear species and magnetic
field strength. The composite emission spectrum therefore contains spatial information.
Reorienting the magnetic field gradient allows one to image concentrations of particular
nuclear species.
III. Passive - Invasive: This category is characterized by requiring direct access to the
brain in order to assess its activity.
Surgical procedures make up this category and very often generate useful data but involve
substantial risk and expense to the patient.
IV. Passive - Noninvasive: This category is characterized by the sensing of source
currents within the brain either through electric potentials on the scalp or extracranial
magnetic field's. In terms of a patients perspective, this category represents the most
desirable of all the options considered.
An electroencephalogram (EEG) is record of the electrical activity of large ensembles of
neurons in the brain. It is obtained while a subject is sleeping, sitting quietly, or during
specific sensory stimulation. The scheme is to place macroelectrodes over the top and
sides of a subjects scalp and measure the electrical potential between active electrodes.
The frequency content of the potentials recorded from the scalp of a normal human
typically vary from 1-30 Hz and are not a result of action potentials but a result of
extracellular current flow associated with summated synaptic potentials in the activated
pyramidal cells. The problem with current noninvasive tests based on EEG measurements
to assess electrical activity abnormalities appears to be with their inadequate spatial
selectivity.
While EEG is the mainstay of passive - noninvasive recording of brain electrical activity, a
relatively new passive-noninvasive technology is emerging for use in imaging the source currents
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of the brain. This technology is built around the magnetoencephalagram (MEG), i.e., a record of
the extracranial magnetic field generated by the brain source currents and has many advantages
over todays competing technologies. In this application, the instrument used to generate images
of brain source currents is built from magnetometers based on superconducting quantum
interference device (SQUID) technology.
SQUID based magnetometers are very low noise devices that can respond to millisecond scale
activity and monitor magnetic fields one billion times weaker than the Earth's magnetic field. This
level of sensitivity and resolution is required because the magnetic fields generated by brain source
currents are typically 100 - 1000 fT in strength and extend from 0 - 1 kHz in frequency.
Clinical implementation of this technology would require a conformal array of SQUID sensors
placed in close proximity to the patients head. The array would then register brain electrical
activity during a monitoring session. By using beamforming and beamsteering techniques, familiar
to phased array antenna technology, in conjunction with an accurate patient specific brain model
one can image source current activity to within a few millimeters, depending on the size of the
sensor array. Most imaging techniques currently being used are based on an idealized dipole
source current model and a layered sphere model of the brain. In reality, however, brain source
currents are distributed throughout regions of the brain. This beamforming and beamsteering
technique is ideally suited to mapping distributed source currents.
Unlike the competing technologies discussed above, brain source current imaging MEG
technology enables one to precisely associate brain function with underlying anatomic structure.
By understanding normal neurological phenomenology it will be possible to quantify abnormal
brain activity and the brain disorders that result. Consequently, this technology will directly
impact the diagnosis of brain disorders such as stroke, epilepsy, Parkinson's disease, Alzheimer's
disease, and head trauma. Furthermore, the ability to quantify abnormal brain activity directly
impacts the development of new drug intervention strategies. Currently it is impossible to
determine drug effectiveness noninvasively. Generally drug effectiveness is judged solely on the
basis of behavioral changes which are notoriously unreliable and may take days or even months to
develop. Moreover, measurements of drug concentrations in the blood stream frequently fail to
indicate the drug concentrations at the brain cells where they are active. The best measurement is
one that monitors the changes in brain activity directly, and preferably one that is passive-
noninvasive. The ability to assess drug efficacy in a timely manner will significantly reduce the
costs involved with bringing an experimental drug to market. Presently the average cost to
achieve this is $231 million and 12 years.
One of the many promising clinical applications of the brain source current imaging technology is
in the identification of the focal point of epilepsy in persons who are candidates for surgical
removal of the epileptogenic region. Current diagnostic procedures, namely EEG, CT, MRI, and
PET often yield inadequate information for accurately determining the location of the
epileptogenic focus within the brain. So the competing technology to diagnostic biomagnetic
imaging is an invasive diagnostic procedure involving surgical intervention using depth electrodes.
These electrodes are inserted into the brain through holes in the patient's skull and the electrical
signals are then monitored for long periods of time, 5-7 days. This procedure obviously comes at
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substantial risk and expense, $20,000-$60,000. Consequently, of the approximately 360,000
persons in the United States that are candidates for epilepsy surgery only a couple hundred a year
are actually treated. If the epileptogenic region can be surgically removed, however, the patient
may become completely free from seizures. Brain source current imaging MEG can decrease the
need for surgical diagnostic procedures in patients with epilepsy by providing preoperative,
noninvasive localization of the epileptogenic focus in three dimensions. It will also minimize the
collateral damage associated with the surgical removal of the epileptogenic tissue. This would
clearly reduce both the direct and indirect costs associated with epilepsy which next to stroke is
the most common neurological disease: about 1% of the population suffers from epilepsy. There
are approximately 55 epilepsy surgery centers throughout the United States and Western Europe
that would directly benefit from this new biomagnetic imaging technology.
Although MEG machines on the market today are large and expensive, it is quite likely that future
machines will be smaller, less expensive, and readily available in a much wider market. This will
permit the dynamic biomagnetic activity of electrically excitable organs (most notably the heart
and brain) to be routinely monitored quickly and noninvasively. The miniaturization of this
technology will permit rapid mass-screening of numerous medical disorders. Many disorders,
when detected in their very early stages, may be treated at a much lower cost and with much less
patient suffering than when they become acute. In this manner, this technology may greatly
reduce medical costs by providing very early detection of disorders long before they become
clinical. Since no physical contact is required with the patient, these machines have the capability
of screening patients rapidly for specific disorders once their capabilities are scaled-up from the
present technological level. This proposed research will result in the machine improvements
necessary to achieve this mass-screening capability. We anticipate that many private companies
would then be interested in producing such machines commercially following a cooperative
research and development activity with our laboratories.
The enormous commercial and research markets for this biomagnetic imaging technology has not
gone unnoticed by foreign governments. In particular, Japan's Key Technology Center (JKTC)
joined with ten domestic firms Hitachi Ltd., Sumitomo Electric Industrial Company Ltd.,
Takenaka Komuten Company Ltd., Shimazu Corp., Seiko, Inc., Daikin Industries Ltd.,
Yokogawa Electric Corp, Toshiba, Shimizu, and ULVAC Corp. to establish the
"Superconducting Sensor Research Laboratory" a new laboratory that will develop SQUID
technology for basic brain research. The specific objective is to develop a 200-channel SQUID
based MEG instrument for noninvasive brain examination. The system will then be used in brain
research including source current imaging and analysis of data. This laboratory was initially
capitalized at 100 million yen, and then recapitalized at 6 billion yen over a six year period that
began in March 1990. The laboratory is funded 70% of budget by JKTC (a satellite bureau of
Japan's Ministry of International Trade and Industry, MITI) and the other 30% by the consortium
of ten companies.
The future of cognitive neuroscience hinges on our ability to study the dynamics of the living
human brain. MEG has become the "new" noninvasive imaging technique that can provide
clinically applicable information on the health of the brain, heart, and neuromuscular system. It
shows promise of being the most important source current imaging technique to impact medical
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imaging since the advent of MRI. It is clear that the United States must not lose the ongoing
technological battle in this area for not only economic competitiveness reasons but also national
security reasons.
III. Problem Statement
This section specifically defines many problems that can be directly addressed with the brain
source current imaging MEG system described in the proposed effort.
A. Neurological problems
The improved ability to extract and pinpoint brain signals using advanced hardware and signal-
processing techniques will have numerous commercial and military applications, only a few of
which can be mentioned here. In the commercial sphere, the most significant anticipated
applications are improved clinical diagnostic tests for functional brain disorders. According to
the Health Care Financing Administration (HCFA), total annual healthcare related spending in
the United States exceeds $400 billion. More than one-third of this total, or $150 billion, is spent
on the diagnosis and care of 72 million Americans affected by neurological and mental health
disorders. The majority of these disorders are functional in nature and are poorly understood.
Despite immense expenditures, the diagnosis and care of those afflicted with these illnesses has
been inadequate because in most cases no direct noninvasive and definitive test exists to
effectively diagnose or monitor treatment. We believe MEG will provide the required test
capability, provided techniques can be developed to readily measure spontaneous and stimulated
brain electrical activity from specific places in the brain that are implicated in specific brain
disorders. This is exactly the goal of our development of the instrumentation and signal
processing techniques described in this proposal, and therefore this work has enormous
commercial potential
To appreciate the range of commercial applications for an advanced neuromagnetometer, we
have selected several significant examples:
1. Epilepsy
The first example is the surgical cure of epilepsy, which is a grossly underutilized therapy. This
is mainly due to the high cost ($20,000 to upwards of $60,000 per patient) and invasive nature
(electrodes are surgically implanted into the brain to record the location of abnormal electrical
activity responsible for the seizures) of the presurgical evaluation. Conservative statistical
projections indicate there are at least 360,000 patients in the United States meeting the criteria
for epilepsy surgery: Their seizures cannot be controlled by drug therapy; they are severely
incapacitated by the disorder, and the brain tissue responsible for their seizures is localized and
could be removed without significant neurological or functional impairment. Yet, only a couple
of hundred epilepsy surgeries are performed annually. MEG is currently being tested as a
noninvasive alternative to the present direct cortical recording techniques, and it shows great
promise. If we can accomplish the improvements in instrument design and signal-processing
capability.that we are expecting in Phase II, MEG should be able to routinely identify the source
of single epileptic events in the brain. This will reduce the cost of presurgical evaluation by an
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order of magnitude and make surgical cure of epilepsy widely available throughout the
developed countries of the world.
Another important medical application is the possibility of assessing stroke damage during the
acute phase when interventional therapy might be administered to prevent irreversible tissue
damage. No noninvasive means exists today to evaluate the spatial extent of reversible brain
damage, and therefore physicians are often reluctant to take risky therapeutic measures without
reasonable assurance that they will benefit the patient. Again, a neuromagnetic brain imaging
system offers the possibility to map out the three-dimensional regions of affected tissue by
focusing on changes in spontaneous brain electrical activity that accompany an ischemic
condition prior to tissue death.
3. Psychiatric Disorders
There is much interest now in the potential use of MEG to assess psychiatric disorders. Some of
these disorders are known to be accompanied by abnormal spontaneous brain electrical activity,
but the association is too tentative for useful diagnosis or therapeutic monitoring. Positron
emission tomography has been shown to have diagnostic potential on the basis of abnormal
patterns of metabolic activity that must have electrical counterparts. Because it relies on
radiopharmaceuticals, PET scanning is an invasive procedure and is unsuitable for routine
testing or therapeutic monitoring. The problem with current noninvasive tests based on EEG
measurements to assess electrical activity abnormalities appears to be with their inadequate
spatial selectivity. The 1000 channel neuromagnetometer should permit the spontaneous
electrical activity of the brain structures known from PET and other means to be affected by the
disorder to be measured directly, thus providing the necessary diagnostic specificity.
4. Head Trauma and Tumor
Head trauma and brain tumor may be associated with regional damage to the brain or to its blood
supply. The proposed whole head functional brain activity imaging system should be able to
detect many signs of brain injury that may not show up on anatomic (MRI or CT) scans of the
head. For example, an injured region may be visualized as a "hole" in the brain activity image.
Also, regions of pathological brain activity such as abnormally slow ("focal slowing") or
abnormally rapid activity, such as may be seen on the boundary of a damaged or compromised
brain tissue. A neuromagnetic image, taken very early after head injury and throughout the
recovery period, may provide immediate feedback on the effectiveness of a particular treatment,
and could lead to improved management of head injuries. The brain imaging system may also
be able to detect signs that indicate tumor or other inflamation of the brain before they show up
in MRI or CT scans. Early detection of brain tumors would have a big impact on reducing
mortality, morbidity, and medical costs.
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5. Learning Disorders
Learning disorders and dementias (Alzheimer's disease, and AIDs dementia, for example) have
been studies primarily by behavioral (psychometric) testing and post mortem examination of the
brain. More recently, tests have been developed to identify biochemical and genetic markers for
some of these diseases. These categories are lumped together in this section for convenience and
due to lack of quantitative evaluation of the roots of the observed behavioral symptoms. The
proposed whole head brain imaging system can permit visualization of the actual brain activity
of each individual while they perform cognitive or memory tasks. By studying and comparing
the way the normal and the pathological brain operate, we may be able to improve
pharmacological brain operate, we may be able to improve pharmacological treatment and
rehabilitation programs.
6. Substance Abuse
Substance abuse represents a serious problem throughout the world. The advanced
neuromagnetometer may be able to detect fundamental differences in brain activity between
those who are prone to substance abuse and those who are not. In addition, it is likely that such
a brain imaging system could be used to noninvasively identify individuals currently using
alcohol or other drugs, without the need for blood or urine tests. Such testing could be of value
for screening personnel involved in hazardous or high-security jobs for which impaired
judgement may have dire consequences. Lastly, our ability to quantitate brain activity may lead
to improved management and treatment of substance abusers.
7. Pre-Operative Evaluation
Functional localization of motor and sensory areas of the brain, including regions serving
language can provide important information needed for planning neurosurgery. Pre-surgical
knowledge of the physical/anatomical locations of brain functions will guide the neurosurgeon in
the surgical approach so as to spare injury to critical regions.
8. Spinal Cord Injury
Spinal cord injuries are often accompanied by motor deficits (paralysis) and loss of sensation for
regions of the body connected below the injured spinal segment. The state of the medical art
being limited, a permanently injured spinal cord cannot yet be regenerated; the connections
between the brain's motor cortex and the muscles are severed. Furthermore, the feedback to the
brain for joint position and muscle tone may also be severed. The proposed neuromagnetic
instrument will have the sensitivity and spatial selectivity to focus on, and extract in realtime, the
signals from the motor cortex of the brain. It is therefore possible to use the brain activity
corresponding to intentional movement to control a prosthetic device to effect that movement.
Although development of a fully portable system is still only conceptual, the principles could be
tested using the 1000 sensor MEG based system.
9. Drug Evaluation
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A final medical example is drawn from psychopharmaceutical treatment and new drug
evaluation. Since it is generally impossible to noninvasively determine the effect of drugs on
specifically targeted regions of the brain, their effectiveness is often judged solely on the basis of
behavioral changes which are notoriously unreliable and may take days or even months to
develop. At best, they are only consequences of the direct action of the drug on the brain.
Moreover, measurements of drug concentrations in the blood stream frequently fail to indicate
the drug concentrations at the brain cells where they are active. The best measurement is one that
monitors the changes in brain activity directly, and preferably one that is noninvasive. There is a
clear and large unmet need that appears to be a promising commercial opportunity for advanced
MEG technology.
B. Basic Neurological Science Problems
1. Cognitive Neuroscience
Cognitive neuroscience has, in the past, relied heavily on localizing brain activity selected at a
specific time latency relative to a signal averaged response. Signal averaging is, of course, useful
for enhancing signal-to-noise ratio, but masks the trial to trial variations in the brain's response.
In addition, as we select longer latencies from the synchronizing stimulus, the brain's response
may have much weaker time-lock (vary in time delay), rendering signal averaging useless. The
more important brain processes that distinguish humans from lower animals - language,
imagination, and problem solving - are not readily locked to any external stimulus and will
require more advanced types of signal processing to extract the desired signals from the
background brain activity.
2. Lie Detection
Present lie detectors are notoriously unreliable because they are unable to test the origin of the
autonomic response resulting in measurable physiological phenomena. The location-specific
recording of spontantaneous brain activity offered by the advance instrument should more
clearly reveal the brain's uncontrollable basic response to interrogation.
3. Man-Machine Interface
Among the potential commercial military applications of an advance MEG system is the
assessment of human mental performance under conditions of high work load. These
measurements may lead to improved design of the man-machine interface by more effectively
conveying essential information to the brain such that the mental work is reduced. A more
speculative but somewhat related application is the possibility that an MEG array focused by
advanced signal processing (adaptive beamforming) to a specific brain site could be used to
control a machine by directed mental activity alone. This could lead to an entirely new interface
between man and machine. Another commercial military application could be screening
personnel for exceptionally demanding jobs. Some individuals are clearly better suited for some
mentally stressful tasks, such as piloting a fighter aircraft in combat conditions, than others. A
reliable early test could save significant money spent on candidates who are unable to complete
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the final stages of their training due to latent inability to meet the demands of the job. Screening
personnel for high security positions could also be an application of military importance.
IV. System Requirements and Design Goals
A. Sensor System Requirements
The sensor array must have full head coverage. The sensors must be spaced closely to one
another (approximately 10 mm center-to-center) so as to maximize spatial accuracy. The
sensors, operating at 4 K should be spaced as close as possible to the head. Present commercial
systems have a 15 to 20 mm spacing. Reducing this to 5 mm through good cryogenic design will
improve signal-to-noise ratio by almost 20 dB. The SQUID sensors must have high linearity,
wide dynamic range, and low noise. All these factors are key to reconstructing images of the
brain's electrical currents. The sensor array must also be able to discriminate against background
ambient magnetic noise, and operate within a hospital environment.
B. Computational Electromagnetics Model Requirements
Imaging the continuous electrical currents of the brain requires high accuracy in computing the
forward solution for magnetic fields and electrical potentials for any distribution of current in the
head. This can be accomplished by creating a finite element model (FEM) from an anatomical
scan (MRI or CT) of the head of each patient. The system must be capable of segmenting the
anatomic image into regions of each tissue type (e.g., scalp, skull, dura, cortex, white matter,
cerebrospinal fluid, etc.). By assigning a conductivity value to each of these regions, an accurate
forward solution may be obtained. The image segmentation should be "turnkey" - that is,
performed with little or no human intervention. The segmentation of an MRI or CT scan into a
three-dimensional model, alone, would have significant medical value in the visualization of
anatomic features.
Segmentation of the brain's cortical surface will further improve the computation of an image of
the brain's electrical activity. First, the cortical layer is the source of the dominant primary
currents and activity (it is the layer of the brain containing the neurons and their dendritic input
connection). No significant sources should lie outside this cortical layer. Next, the electrical
current vector is known to flow at right angles to the cortical surface. By knowing the local
normal vector to any part of the cortical surface, we can reduce the number of unknowns in the
image to just one - the current amplitude. Without this normal vector, there are three unknowns
for the X, Y, and Z current amplitudes.
C. Supercomputer Requirements
The typical volumetric MRI scan is composed of an array of 256 by 256 by 128 voxels (volume
picture elements), each with a dimension of I by 1 by 1.5 mm. Segmenting these 8.4 million
picture elements requires a computer with a large memory capacity and high speed. Once the
image is segmented, a finite element model can be constructed. Assuming a model volume of
about 3000 cm3, and a required localization accuracy of less than 0.5 cm, it is obvious that the
FEM must contain at least 24,000 elements. Computation of the forward solution from this FEM
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will require large memory capacity and high speed. In a clinical setting, it is desirable to be able
to compute complete images in under 5 minutes. This "benchmark" is roughly the time it takes
to process an X-ray film. Computation of spontaneous brain activity at a specified location
(simulating an invasive depth electrode) must be computed in realtime.
D. 4th Generation Brain Activity Imaging System Design Goals
The overall goal of this aspect of the project is to develop an instrument capable of generating a
moment-to-moment image of the brain's electrical activity. To accomplish this, the instrument
must measure the magnetic fields generated by the brain over the entire head with high spatial
resolution. Based upon a sensor spacing of approximately 1 cm, this will require on the order of
1000 independent SQUID sensors.
Using present manufacturing practices, it is impractical to scale the current MEG system designs
to 1000 channels. Analog dc SQUID sensors require a minimum of four wires (excluding the
superconducting connections to the sensing coils) - two for bias and two for modulation and
feedback - to connect with their room temperature flux-locked loop (FLL) electronics. These
connections, which go from 4.2 K to 300 K represent a significant thermal load to the SQUID
dewar/refrigeration scheme. Furthermore, it will be necessary to address the cross-talk between
channels arising from the close proximity of these leads to one another. Even if we were to
presume that such a system could be built using current techniques, the cost - on the order of
$50,000 per channel - would make a 1000 channel system unmarketable. Clearly, in order to
engineer the next-generation MEG system, we must address questions of cost and
manufacturability.
Experimental all-digital thin film dc SQUID magnetometers have been demonstrated by several
laboratories. The most noteworthy example was developed by Fujitsu, implementing the entire
flux-locked loop on a single superconducting integrated circuit chip. This digital SQUID
requires only three wires - bias, pulse output, and common. Since the bias and pulse output
lines may be digitally multiplexed, a practical all-digital SQUID can significantly improve the
thermal design by reducing the number of wires per channel going from 4.2 to 300 degrees K,
and reduce crosstalk by virtue of a digital rather than analog output. The all-digital design also
eliminates much of the room-temperature electronics, including the data acquisition subsystem.
Furthermore, the input (sensing) coils would be integrated "on-chip," eliminating the need for
superconducting interconnects, thus increasing reliablility. Development of a single chip digital
SQUID magnetometer could be the key to making large array MEG systems commercially
practical.
The cryogenic support of the current generation of commercial MEG systems consists of a
dewar in which the dc SQUIDs and sense coils are immersed in a bath of liquid helium. The
evaporation of liquid helium provides the refrigeration for the SQUIDs, which must be
maintained below 10 K to be superconducting. A helium dewar system requires periodic
replenishment of the liquid cryogen, and also poses limits to the degree to which the dewar and
SQUIDs may be tipped in order to position the system around the head. Closed-cycle
refrigeration of a dc SQUID magnetometer, using a Joule/Thompson heat exchanger has been
successfully demonstrated using commercially available refrigeration components. In order to
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keep the proposed 1000 channel neuromagnetometer as small as possible, it will be necessary to
develop a low-noise closed-cycle refrigeration scheme - a cryocooler - eliminating the need
for a liquid helium reservoir large enough to immerse all sensors.
The Earth's magnetic field is approximately 1 billion times larger than the brain's magnetic
signals, which are about 5 x 10-13 T peak-to-peak. In a typical city hospital, electrical
machinary and ferrous objects moving in the Earth's magnetic field result in magnetic noise on
the order of 10-7 T peak-to-peak. Many commercial neuromagnetometer designs include a
magnetically shielded room as part of their system. This shielding attenuates the magnetic noise
to levels low enough for the brain's MEG signals to be seen. However, a magnetically shielded
room adds about $500,000 to the cost of an MEG system. Canadian Thin Films (CTF) has
demonstrated a SQUID neuromagnetometer that does not require a shielded room. Using wide
dynamic range digital SQUID electronics, they use noise reference channels to sample and
subtract the ambient magnetic noise. A wide dynamic range design and adaptive noise reduction
must be explored in the 4th generation MEG system design.
What does one do with 1000 channels of information? The traditional approach borrowed from
EEG - displaying individual channel time series on a strip-chart recorder - is impractical.
Furthermore, conversion of the MEG data into single and multiple equivalent current dipoles
(misleadingly referred to as "magnetic source imaging" by some companies) discards most of
the information obtainable from a large array MEG system. To address this, we propose using
beamforming and beamsteering methods, a procedure borrowed from the processing used for
large phased array antennas in radar and radio. This technique will permit us to estimate a three
dimensional image of the instantaneous electrical currents throughout the brain. In addition, the
electrical activity in any location within the brain could be examined as if an invasive depth
electrode had been implanted there.
In order to compute accurate high-resolution tomographic images of brain activity, the precise
shape of the head, together with that of each tissue layer (scalp, skull, dura, cerebral cortex, etc.)
must be known. Thus "turnkey" software must be developed for automatically segmenting MRI
or CT images of the head into a finite element computer representation of each different tissue
layer. It is this finite element model that enables us to compute the magnetic fields and electrical
potentials due to the electrical activity generated by the brain. It is expected that a low-end
parallel supercomputer will be required in order for image segmentation and FEM compution
time to take less than 5 minutes.
Computation of an image of the source current distribution using the measured magnetic fields
and will also be programmed on a supercomputer. A time-moving image of brain activity will be
computed frame by frame. The source current images will be "fused" with the anatomic image
of the brain, thus enabling the viewer to see the relationship of the brain activity with its
corresponding anatomic structures. A graphics workstation will be used to permit flexible
display of the fused images. Selection of an anatomic coordinate from the brain image will allow
selective display of the time-changing brain activity waveform that was estimated for that
location.
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Clearly, the development of such an advanced neuromagnetometer will require a systems
engineering approach. Developing processes for improved sensors and cryogenic support are
important, but don't constitute a whole system, whose design will guide potential manufacturers
in production techniques needed for the next-generation neuromagnetometer.
V. Proposed Effort
The proposed effort consists of two phases. In the first phase we will undertake risk reduction
experiments that will lead to the development of a small-scale near realtime MEG based imaging
system. While this instrument will not give simultaneous full-head coverage, it will constitute a
proof-of-principle instrument and will enable the second phase of the proposed effort. In the
second phase we will implement the full-scale instrument design that minimizes the associated
risks as identified in Phase I. The second phase will end with a full-scale demonstation of a near
realtime MEG based imaging system.
The configuration of the full-scale MEG imaging system is shown in Figure 1. The cryogenic
assembly is positioned over the patient's head. It contains the array of SQUID magnetic-field
sensors, which spans the entire scalp and must be closely aligned with it, along with the cryogenic
pickup electronics. An alignment subsystem monitors and adjust the position of the assembly
relative to the head. The low-level signals from the pickup coils are brought out to a bank of
room temperature amplifiers, then sampled and digitized by the acquisition subsystem to create
digital data files which are stored on a host computer. The host provides a user interface for
control of system parameters such as amplifier gain and sampling rate. It also serves as a front
end to a parallel supercomputer which calculates the extracranial magnetic fields due to a point
source using the electromagnetic brain model (constructed from auxiliary data such as MRI scans)
and uses these results, along with the SQUID data, to compute maps of brain activity in space and
time. The host, under user control, post processes the maps and feeds them to a display
subsystem. The system software also provides for system calibration using test inputs developed
from SQUID measurements of simulated brain-like signal sources, i.e., phantom measurements.
Figure 1. System configuration
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Phase I of this project will include a detailed, end-to-end proof of principle. We will develop
prototype computer codes for electromagnetic brain modeling and activity mapping, and we will
acquire the supercomputing resources needed to run these codes rapidly. The algorithms will be
based on realistic models of brain signals derived from patient specific brain data. Analyses and
simulations will establish the capabilities, such as number of channels, sensor spacing and noise
floor, that the full-scale MEG system will need to make useful whole-brain maps of the
phenomena of interest.
To facilitate brain data collection necessary for Phase I proof-of-principle experiments, a state-of-
the-art MEG system (37 channels or more) will be procured and installed at the VA Medical
Center in Albuquerque. Although such a system does not provide simultaneous whole-head
coverage, nor adequate sample density to measure all types of brain activity in a -clinical setting, it
is valuable as a source of research data from which space-time profiles of important brain events
can be generated. Today's state-of-the-art models of brain activity are much too crude to yield
predictions at this level of detail, and so cannot serve as a guide to MEG system design. Once the
empirical profiles are found, they will be expressed as computational models suitable for analysis
and simulation.
A computational electromagnetic model of the brain is needed to predict what data a signal of
known profile will produce in a MEG sensor array of known configuration. This is referred to as
a "forward" model, and is a necessary part of the "inverse" model which reconstructs the brain
activity from a given set of sensor data. The brain signals can be thought of as current sources
("primary currents") which induce "secondary" return currents that obey Ohm's law. These
currents produce magnetic fields as described by the Biot-Savart law; each SQUID sensor
measures a component of the total field at a point in space. The task of the forward model is to
compute the magnetic fields, given the primary currents. In most models, the head is treated as a
set of concentric spheres, for which the field can be expressed by an analytic formula. The errors
in such a model are unacceptable in a system that is to localize the measure the primary sources
with high accuracy, because they cause high-performance inversion algorithms to fail. With a
realistic electrical model of the head, no analytic solution is available; the field must be computed
numerically. As part of the proof of principle, we will develop codes to compute a 3-D finite-
element model tailored to the shape of each patient's head, as derived a priori from auxiliary data
such as an MRI scan. The code will be validated, first through tests on standard shapes with
known analytic models, and later through comparison to data collected on phantoms. An existing
parallel supercomputer, belonging to Dept. 9735 at Sandia, will be upgraded as necessary to run
the codes at a speed sufficient for large-scale simulation and testing.
To provide clinically relevant data requires both timely and accurate patient specific brain
information. The ability to accurately image brain source currents is dependent on having an
accurate forward solution. The forward solution consists of solving for the extracranial magnetic
field generated by a localized source current within a brain model. In order to generate an
accurate forward solution the brain model will be generated directly from patient specific
anatomical data gathered through a standard MRI session. During Phase I and using the MRI
data we will demonstrate that (1) a detailed finite element mesh of the brain can be constructed
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and (2) the appropriate electrical characteristics of the brain media can be estimated. To
accomplish this in a timely manner will require an automated data segmentation procedure that
can accurately extract boundaries of the five different media which comprises the brain. The
multiple MRI data segmentation tasks will be accomplished through a static decomposition on a
parallel supercomputer for high parallel efficiency. Necessary electrical properties of the various
brain media will be extracted directly from the MRI data. Once the boundaries and electrical
characteristics have been determined a 3-D fmite element mesh, the brain model, will be
generated. Within the brain model one can now place a localized current source. The extracranial
magnetic fields generated by this current are then computed using the parallel supercomputer and
used to guide the beamsteering algorithm to a specific site within the actual brain (MEG) data
space. By moving the current source around in the brain model one can localize, i.e., map the
actual brain source currents contained within the MEG data.
We will undertake analysis and computer simulations to assess the usefulness of an MEG sensor
array as a noninvasive probe of brain activity. Such a probe must take accurate measurements
over time of currents within a small, localized portion of the brain. Interfering signals from other
parts of the brain must be suppressed, along with signals from sources outside the head such as
RF interference from electronic equipment. The effect of random noise within the MEG sensors
must also be kept low.
Given a MEG based imaging system, the key to accurate localization of brain activity then
depends upon the signal processing techniques implemented. The signal from the desired region
appears at each of the MEG sensors with a strength that depends on its location within the brain.
The signal processing algorithm must combine the sensor outputs in such a way as to reproduce
the desired signal while suppressing noise and interference. It relies on the forward model of
sensor gain vs. location in making the combination. The model is adjusted to an individual patient
using the same auxiliary data used in finding the head shape, to create a "brain atlas" showing the
region of possible signal sources. To avoid the high cost of human interpretation, the atlas must
be created by an automatic process involving segmentation of the auxiliary images to identify
regions composed of tissues of different types. This is a classic computing problem for which a
variety of promising approaches exists. Guild members from the University of New Mexico will
develop image segmentation methods specific to the MEG problem. These will be combined with
the computational electromagnetics codes to create a system capable of solving the forward
modeling problem rapidly.
Given a forward model, the "inverse" problem of reconstructing the brain activity from the MEG
sensor outputs is solved by computing an ensemble of weighted linear combinations of the sensor
outputs. Each combination is an estimate of the activity vs. time in a small region of the brain,
and its weights are chosen to select activity in that region while suppressing activity elsewhere in
the brain and interference from outside the head. The problem of choosing the weights is
analogous to the problem of beamsteering in array antennas. Its solution is aided by the fact that
over short periods of time, only a small fraction of the region of signal sources is active. This
makes possible the use of concepts from the theory of adaptive arrays, in which the location of
interfering sources is estimated from the data and the array weights chosen to direct antenna
pattern nulls at the interfering sources. Techniques of this kind have been used successfully to
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enhance data from existing MEG systems. Guild members from Sandia, the Veteran's
Administration, and other laboratories will develop algorithms for the inverse problem on large
arrays, using brain data to refine the reconstruction model. These codes, combined with the
forward solution codes, will make up the prototype of an end-to-end capability to compute maps
of brain activity vs. space and time from MEG and auxiliary input data.
As the algorithms are developed, they will be incorporated into analyses of the performance of
candidate MEG sensor configurations. Simplified models will be used to identify the most
promising candidates, then detailed simulations will be used to choose the configuration preferred
for full-scale development.
A. Hardware System Development
The proposed design approach will work from the bottom up and from the top down
simultaneously. Clinical information obtained from the Phase I study using existing 37 channel
MEG machines and improved source reconstruction algorithms will be used to predict the
minimum sensor density necessary to detect various brain functions and to diagnose various
disorders. While this is underway, a second study will determine the maximum number of brain
sensors which may be supported by a fixed level of supercomputing support. Although the
optimal number of brain sensor channels will be determined from these studies during the first
phase, we anticipate the optimum number will be about one thousand. These studies will consider
two different operating scenarios; one which provides near realtime information with no more
than a 5 minute delay, and the other which accumulates data on the evoked cortical response due
to repeated stimulation. The first mode of operation, which will be genuinely new for MEG,
should prove useful in rapid mass-screening for particular disorders. It should also prove useful
during useful during certain surgical techniques. The second scenario will expand the capabilities
of previous MEG machines, providing greater utility to drug action studies and to the brain's
functional mapping. Although these initial designs are optimized for brain research, the design
will remain flexible so that it may be re-deployed for other research, such as heart and fetal
studies.
B. Machine Design Issues
Today, commercially available MEG machines are limited to a maximum of 37 channels.
Canadian Thin Films, Inc. plan to introduce a 90 channel system soon, and Neuro Mag, Ltd. of
Helsinki, Finland have recently reported their successful testing of a 122 channel system. Japan's
MITI are attempting to develop a similar machine with at least one hundred channels designed for
full-cortex coverage. Considering the current state-of-the-art it is apparent that this proposed
1,000 channel MEG system will represent a dramatic increase in the overall system complexity.
As discussed below, this increase in system complexity will mandate a genuinely new system
architecture which permits a much more dense packing of sensor channels, and which utilizes
novel new cryogenic support designs which will permit low-noise operation in any orientation of
the MEG sensor array. As such, we propose a number of risk reduction experiments during the
first phase designed to define the optimal approach for increasing the density of sensor channels in
the proposed super-MEG machine. Two different technical approaches will be pursued to
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optimize the SQUID and sensor configuration initially. The first, lower-risk approach will
determine the optimal method of close-packing conventional thin-film analog SQUID amplifiers
and their associated micro-lithographic sensor coils at the density required in this super-MEG
machine. The second approach, entailing higher risk and a much higher potential benefit, will
pursue technical improvement of a new class of digitally biased SQUIDs which have only recently
been developed, primarily by Fujitsu in Japan. We anticipate that this second approach will
rapidly close our existing technical deficit, relative to Japan, in this emerging new SQUID
technology, which should prove useful in many civilian and military applications, as well as in the
proposed MEG work. After 15 months, the optimal SQUID and sensor technology will be
selected and integrated into the overall super-MEG system design. These risk reduction
experiments, together with others related to the system's cryogenic and thermomechanical design,
are described below.
C. SQUID Risk Reduction Studies
As more sensors and SQUID amplifiers are packed into a limited surface coverage about the
human cortex, problems associated with channel cross-talk and bias/feedback sub-system
interference become a major limitation to continued system expansion. Recently Fujitsu has
begun an extensive program, coordinated through MITI, focused on the development of digitally-
biased SQUIDs in which all feedback and readout functions are facilitated on the same integrated
circuit as the SQUID and sensor coil. Although this technology could solve many of the high-
density packing problems mentioned above, overall noise level and other system integration issues
greatly limit its utility at this time. Improvement of this technology for incorporation into the
super-MEG system is considered high-risk, however, the remaining technical developments
necessary to make this technology viable seem readily achievable. A series of risk reduction
experiments designed to utilize these new SQUID devices will be pursued, together with less risky
experiments which use conventional analog SQUIDs with room temperature biasing and feedback
electronics. At the end of these experiments, and at the culmination of the first phase of this
proposed research, we anticipate that the final super-MEG system design will utilize an optimized
hybrid of these two SQUID design concepts.
Numerous domestic manufacturers of thin-film SQUIDs are capable of producing the channels
which utilize conventional, analog SQUID technology. Firms such as IBM, Quantum Design,
Conductus, BTi, Hypres, and possibly others would be potential contractors for this aspect of the
work. In order to minimize the SQUID cross-talk at our required high density of sensor packing,
we will issue a contract to at least one of these firms (during the first phase) to produce a
miniature fifty-SQUID sensor array at this packing density. This will permit the materials and
micro-lithographic designs to be optimized to minimize cross-talk and feedback channel
interference to the incoherent noise level. These small contracts executed during the first phase
will greatly reduce the technical and business risks associated with the super-MEG machine
development during the second phase.
The higher-risk digital SQUID technology will also be pursued aggressively during the first phase.
TRW owns the basic digitally-biased SQUID patents within the United States, and as such we will
attempt to team with them in all such efforts. Fujitsu, with extensive funds from Japan's MITI,
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have taken the world lead in digital SQUID technology. Fortunately, Fujitsu has been very open
with this technology through numerous publications. Fujitsu's scientists seem willing to
collaborate with their USA colleagues, so we propose to place a physicist at Fujitsu's
development laboratories to work with their lead physicist, Dr. H. Fujimoto, during the first phase
of this development. We know of two physicists, both fluent in Japanese and USA citizens, who
may be interested in this position at Fujitsu through a contract with their current employers. This
physicist may act as a technical liaison, conveying technical information from the MITI
laboratories in Japan to firms in the USA such as Sandia and TRW. Once the basic self-contained
digital SQUID sensor has been developed, we will study the way in which they may be close-
packed, in a manner similar to the study with analog SQUIDs described above.
D. System Integration Developments
The first two sets of risk reduction studies outlined above involve the optimization of the basic
SQUID and sensor design. In essence, this aspect of the system development centers on
optimizing the basic "building block". System integration and cryogenic support studies will also
be conducted during the first phase in order to determine the optimal method of thermo-
mechanical support of the very large array of sensors in the super-MEG machine.
Recent advances in closed-cycle cryogenic refrigeration technology have resulted in dramatically
longer intervals of highly reliable continuous operation (typically 20,000 hours), and in astounding
cost reductions, both in purchase price and operating costs. New cryogenic designs which
integrate the SQUID and sensor array into a plenum structure which serves as the closed-cycle
refrigerator's lowest temperature heat exchanger will permit operation of the super-MEG machine
in any orientation. This will greatly increase the clinical utility of these machines.
Present day MEG machines locate the fifty liters of liquid helium, which maintain the SQUIDs and
sensors in their superconductive state, directly over the patient's head. This primitive cryogenic
design, which Newsweek referred to as the "Hair dryer from Hell" in their April 20, 1992 issue,
uses gravity to stabilize the liquid helium under its vapor throughout the clinical measurements.
Any repositioning of the apparatus above the patient's head requires a cumbersome relocation of
this large apparatus on a hefty overhead supporting transit system. Such motion inevitably creates
a sudden increase in the liquid helium boil-off rate, resulting in a loud hissing sound as the cold
helium vapor escapes from the system's check valves. This process is disruptive even to healthy
humans, and it is often absolutely terrifying to patients afflicted with major psychiatric disorders
such as paranoid schizophrenia. The new cryogenic support systems to be incorporated into the
super-MEG machine will operate silently in any orientation. The space saved by removing the
liquid helium storage volume should permit the thousand-channel super-MEG system to occupy
less overhead volume than existing 37-channel systems.
E. Thermo-Mechanical Risk Reduction Experiments
The development of this integrated cryogenic support architecture will involve the construction of
micro-lithographic arrays of SQUIDs and superconducting sensor coils which are supported by
thousands of thermally-conducting electrical feed-throughs protruding from the refrigeration
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plenum. These feed-throughs will provide the electrical contracts to the SQUID and sensor
arrays, together with the cooling necessary to maintain these arrays in their superconductive state.
A fifty-channel prototype of this design at a packing level equal to the super-MEG design, shall be
developed during the first phase of this effort to reduce the technical and business risks during the
full-scale, second phase construction. We anticipate that these risk reduction experiments,
together with the overall integrated design development, will be performed within Sandia.
The closed-cycle refrigerator which will maintain the integrated plenum and SQUID/sensor arrays
at or below 5 Kelvins will be located away from the immediate clinical environment. The
refrigeration cold head will be located about four meters from the super-MEG array, possibly in
the pipe chase adjacent to the MEG room. An evacuated and super-insulated flexible hose shall
connect the refrigeration cold head to the clinical MEG assembly. The refrigeration cold head will
have a total mass of about 15 kg. It shall be supported by a 100 kg helium compressor which may
be located an arbitrary distance from the cold head, say in a utility shed. Concepts similar to this
design have been successfully proven in other superconductive device applications within Sandia,
and as such no first phase risk reduction studied need be undertaken.
The optimal design for the refrigeration cold head is evolving rapidly at this time. For this reason
we shall evaluate numerous competitive designs during the first phase to optimize the final
cryogenic system's reliability and efficiency. Manufacturers of these new and vastly improved
closed-cycle 5K refrigerators within the USA include Boreas, RMC, Tristan, CryoMech, and
possibly others. Since the superconductive electronics dissipate little to no heat while they
operate, this super-MEG design requires only a modest amount of cooling power to maintain a
temperature below 5K. Hence the closed-cycle refrigeration development aspects involve only a
reliability study and little to no additional engineering development.
Figure 2. Proposed Project Organization
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In Phase II, we will design and fabricate a full-scale MEG array system, capable of localizing and
measuring electrical signals over the whole brain with the maximum precision allowed by the laws
of physics. It will contain on the order of 1000 SQUID sensors, in an array spanning the entire
scalp. The computational models, understanding of brain activity, and sensor technology
developed in Phase I will serve as the basis for the design. Once completed, the system will be
installed at the VA Medical Center in Albuquerque to serve as a national resource for research
into brain function and brain disorders.
The fifty-channel prototype sensor built under Phase I will be installed at the VA at the start of
Phase H. Collection of brain data will continue throughout this phase. The fine spatial resolution
in this system will make it possible to extract more detailed and accurate signal profiles than those
found in Phase I. A library of profiles will be incorporated into the computational model as part
of the initial operational capability for the full-scale system.
The computational model and mapping algorithms will be revised based on the experience of
Phase I. We will acquire a parallel supercomputer, of the highest performance commercially
available, to run the codes. The software configuration will make use of the parallel computer's
ability to allocate processing power dynamically as the task load changes. The forward model will
be made more detailed (size increased from 24,000 elements to approximately 1 million) to
achieve the necessary model quality at high spatial resolution. The inverse model will be revised
and recorded as necessary to accommodate the large number of sensor channels. All the codes
will be integrated to create a system capable of computing MEG scan results in a timely manner
(one hour from start of auxiliary scan to finished output).
The hardware design of the full-scale sensor will be finalized early in Phase II, with the rest of the
time devoted to fabrication, assembly and integration. Fabrication of microelectronic components
will be done at Sandia's Microelectronics Development Facility, at contractors facilities, or some
combination. The cryogenic subsystem will be built at Sandia, and assembly and integration will
be done there.
VI. Proposed Costs and Schedule
This section gives the proposed costs and schedules. The effort would be managed by Sandia
National Laboratories with the Veteran Administration MEG Laboratory being a core laboratory
along with Sandia. Sandia will develop contracts with the University of New Mexico to work in
image analysis and to advise on some aspects of neurological sciences, Los Alamos National
Laboratory for basic sensor research, the University of Houston for computational
electromagnetics, the University of Arizona to consider machine interfaces for surgical
procedures, and other industrial entities for both sensor and computational electromagnetics
research.
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The proposed funding profile is as follows:
A. Phase I
1. Core Laboratories
a. Sandia National Laboratories
1) Supercomputer Upgrade
2M
2) Inital EM Brain Model Developement
3M
3) Initial Sensor Array
4.5M
9.5M
b. Veterans Administration
1) MEG Acquistion and Installation
3M
2) Research
0.7M
3) MRI Time
0-IM
3.8M
2. Universities
a. UNM (EECE Dept.)
300K
b. University of Arizona (Neurology Dept.) 500K
c. University of Houston (EECE Dept.)
100K
900K
3. Others
a. Ochsner's Clinic
200K
b. Los Alamos National Laboratory
(Device Research)
500K
c. McDonnell-Douglas (CEM Consultant)
400K
d. IBM (SQUID Research)
500K
e. TRW (SQUID Research)
500K
f. Other consultants
300K
2.4M
Total Phase I - 16.6M
B. Phase II
1. Core Laboratories
a. Sandia National Laboratories
1) Supercomputer and Workstation Acq. 8M
2) Final EM Brain Model Development 6M
3) Final Sensor Array 14M (includes subcontracts)
b. Veterans Administration (Research) 2M
2. Universities
a. UNM (EECE Dept.) 600K
Approved For Release 2000/08/08 : CIA-RDP96-00789R003300190001-5
Approved For Release 2000/08/08 : CIA-RDP96-00789R003300190001-5
b. University of Arizona (Neurology Dept.)
1.5M
c. University of Houston (EECE Dept.)
200K
2.3M
3. Others
a. Ochsner's Clinic
400K
b. Los Alamos National Laboratory
(Device Research)
1 M
c. McDonnell-Douglas (CEM Consultant)
600K
d. Other consultants
1.1 M
3.l M
Total Phase II - 35.4M
Total 3 year program cost $52M
Approved For Release 2000/08/08 : CIA-RDP96-00789R003300190001-5
Approved For Release 2000/08/08 : CIA-RDP96-00789R003300190001-5
Appendix: Domestic and Foreign Capabilities
A. Existing U. S. Capability--Manufacturers
BTi, San Diego, CA
Founded in 1970 as S.H.E. Corporation, BTi introduced the first commercial SQUID sensor and
electronics. In 1980 they introduced the first commercial dc SQUID system, BTi is considered the
world leader in commercial SQUID systems, supplying SQUID sensors, electronics and dewars
for laboratory use along with geophysical magnetometers and biomedical gradiometers. BTi's
most complex SQUID system is a 37-channel gradiometer array for biomagnetism that includes 8
additional SQUID channels for electronic noise cancellation ($2,200,000) with a system noise
10 fT/. BTi has also delivered single channel dc SQUID biomagnetometers operated by a closed
cycle refrigeration system (hybrid Gifford-McMahon/Joule-Thompson) with a system noise 20
fT'/. Although BTi has a DARPA/ONR contract to do research on and fabricate high Tc SQUIDs,
BTi's current thrust is purely biomedical. In July 1989, BTi went public, with a market valuation
of - $50,000,000. In January 1990 Sumitomo Metal Industries, Ltd. of Tokyo became BTi's
Asian distributor. As part of that arrangement Sumitomo purchased 12.9% of BTi, along with
two 37-channel biomagnetometers to be placed at development sites in Japan. BTi currently
employs 135 people of which half are involved in the development of SQUID devices. BTi
operates a subsidiary in Aachen, W. Germany (S.H.E. GmbH) to handle European sales and
service. Sales for 1989 were $8,100,000, with a projected growth of 30% annually.
Quantum Design, San Diego, CA
Privately held, QD was founded in 1982 by four former S.H.E. employees supplying SQUID
electronics and systems. Their major product is a SQUID susceptometer, accounting for more
than 80% of their sales. QD has developed 200 MHz rf SQUID electronics that achieve
35 mF0/ (using BTi rf SQUID sensors). They also manufacture BTi style 20 MHz electronics
with a noise level of 100 mF0/. A subsidiary, Quantum Magnetics, is the R&D arm of QD being
primarily concerned with new product development and custom systems. QD currently buys rf
SQUID sensors from BTi, but now has capability to produce dc (and rf) SQUIDs of their own
design. One interesting feature of their design is the ability to desensitize the SQUID sensor by
factors of 100 or more (e.g., to 10-26 Joules/Hz). Custom systems supplied by QD include a
SQUID magnetometer with 3 m spatial resolution, systems for detection of corrosion currents and
a 6-element airborne gradiometer system. QD is the subcontractor to IBM on NCSC, Panama
City 8-element array refurbishment. As part of this project, they have developed compact dc
SQUID electronics that operate at the 5 mF0/ level (using BTi dc SQUID sensors).
Current research activity (SBIR funded, pointing towards commercial exploitation) include
development of magnetometers for corrosion measurements (NDE) and SQUID NMR for
explosives/drug detection. Estimated revenues for 1989 were $10,000,000. These revenues are
not expected to increase because of market saturation of their principle product, the model
MPMS SQUID susceptometer. QD currently employs 80 people. European sales are handled
through S.H.E. GmbH.
Approved For Release 2000/08/08 : CIA-RDP96-00789R003300190001-5
Approved For Release 2000/08/08 : CIA-RDP96-00789R003300190001-5
2-G Enterprises, Palo Alto, CA
Basically a garage shop outfit, they have two decades experience in constructing SQUID systems.
Their principle product is a rock magnetometer. They are also a manufacturer of SQUID systems
to various government agencies. Normally, they supply their own rf SQUID sensors and
electronics, but have supplied systems with BTi SQUIDS. Estimated revenues for 1989 were on
the order of $ 1,000,000.
Systems Integrators
SQM Technology, San Diego, CA
Spun off from Physical Dynamics, SQM is a small company with only a few persons devoted to
SQUID systems. They have constructed SQUID magnetometers for geophysical research, most
often in hostile environments (arctic, underwater, etc.). Current research interests included
SQUID NDE. They often use outside vendors (QD, BTi) for major subsystems. Current research
support comes from SBIR grants (DARPA, ONR and DoE). Annual revenues are estimated to be
less than $1,000,000.
Dynamics Technologies, Torrance, CA
Funded by a DoE SBIR phase H grant, they built a single airborne 6-element system. The
magnetometer array consisted of 3 first derivative vertical () gradiometers plus 3 orthogonal
magnetometers for electronic noise cancellation) using QD 200 MHz electronics. The probe was
constructed by Quantum Design. Gradient sensitivity
-10,000 fT/meter (3 x 10-3 g/ft), mostly due to motion-induced noise. Apart from the SBIR
grant, annual revenues are minimal (