diamond sensors for brain imaging - mit · the human brain is the most complicated biological...
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Diamond Sensors for Brain Imaging
Dr. Danielle Braje
MIT Lincoln Laboratory
6 March 2018
Revolutions in Biotechnology
This material is based upon work supported by the Assistant Secretary of Defense for Research and Engineering under Air ForceContract No. FA8721-05-C-0002 and/or FA8702-15-D-0001. Any opinions, findings, conclusions or recommendations expressed in this material are those of the author(s) and do not necessarily reflect the views of the Assistant Secretary of Defense for Research and Engineering.
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© 2018 Massachusetts Institute of Technology.
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Quantum Sensing - 2DAB 03/06/18
Brain Science
The human brain is the most complicated biological structure in the known universe. We’ve only just scratched the surface in understanding how it works – or, unfortunately, doesn’t quite work when disorders and disease occur.
- NIH Director Francis S. Collins, M.D., Ph.D.
China Brain Project
South Korea Neuroscience
European Union
Japan
Quantum Sensing - 3DAB 03/06/18
Brain Science
Neuronal activity is at the heart of this complex and nearly intractable system
These small electrical impulses may hold the key to memories, consciousness, and the cure to diseases
And may be the key to brain-machine interfaces
Parkinson’s Disease
Epilepsy
Traumatic Brain InjuryAutistic Spectrum Disorders
Post-Traumatic Stress Disorder
Alzheimer’s Disease Stroke
Huntington’s Disease
Quantum Sensing - 4DAB 03/06/18
Non-Evasive Neuronal Imaging
Electroencephalography
• Measures electric field
• Resolution of cm
• Localization accuracy susceptible to conductivity profile variations
• Localizes tangential, radial, and deep sources
>100,000 worldwide
E-Field
Quantum Sensing - 5DAB 03/06/18
Non-Evasive Neuronal Imaging
Electroencephalography
• Measures electric field
• Resolution of cm
• Localization accuracy susceptible to conductivity profile variations
• Localizes tangential, radial, and deep sources
*Magnetoencephalography invented at MIT by David Cohen
Magnetoencephalography*
• Measures magnetic field
• High resolution of mm
• Localization robust to details of tissue, fluid, and bone
• BUT localizes only tangential sources
MEG sees less than EEG, but sees it better
>100,000 worldwide~200 worldwide(29 in USA)
E-Field
B-Field
Quantum Sensing - 6DAB 03/06/18
Magnetoencephalography (MEG)
Solve biomagnetic inverse problem
(localize current sources)
Magnetic fields
Bulk neuronal activity
Record with sensor array
Action currents
Real-time 3D mapping of neural activity Spatial resolution: mm-scaleTiming resolution: sub-ms
Commercial MEG at Mass General Hospital Martinos Center
Quantum Sensing - 7DAB 03/06/18
Conventional Magnetoencephalography Barriers
High cost of MEG limits widespread use
• Cryogenic Sensors• Rigid Helmet
• High Cost• Shielded Room
MEG=Magnetoencephalography
Quantum Sensing - 8DAB 03/06/18
Room Temperature MEG
CAD of MIT LL Apparatus
MIT-LL Proposed Room-Temperature MEG with Diamond Sensors Overcomes Traditional Barriers:
• Cryogenic Sensors• Rigid Helmet
• High Cost• Shielded Room
NV diamond-based sensors are optimized as a room-temperature alternative to SQUID-based, cryogenic, commercial sensor arrays
Current MEG Facility Requirements Hamper Widespread Clinical Applications:
• Room Temperature Sensors
• Flexible Helmet• Low Cost• Small Shield
Quantum Sensing - 9DAB 03/06/18
NV Sensor Advantages over Conventional MEG
http://kurage.nimh.nih.gov/library/Main/brainmovie.gif
5 cm
Microwavedelivery
Diamond
3 mm
Laser
Conventional SQUID MEG
NV Sensor
• Close proximity to head ~100 fT field
• Room temperature• Full vector field
• Standoff detection ~ 10 fT field
• Cryogenic sensors• Detects only radial field
0.3 cm
Quantum Sensing - 10DAB 03/06/18
Quantum Systems in Diamond
12C
12C12C
12C
12C12C
12C
12C12C
12C
12C12C
12C
12C
12C
12C12C
12C
3.6 Å
NaturalDiamond
1 mm
Engineered Diamond
1 mmSensitive to
Magnetic Field
14N
Quantum Sensing - 11DAB 03/06/18
Nitrogen Vacancy (NV) Diamond Physics
Technical Approach• Initialized optically
• Manipulated with RF
• Long coherence at room temperature
Excitedstates
Groundstates
Intersystem crossing
Green optical
excitation
±1
0
12C
12C12C
12C
12C12C
12C
12C12C
12C
12C12C
12C
12C
12C
12C12C
12C
14N
3.6 Å
637–800 nm fluorescence
2.87 GHz
Quantum Sensing - 12DAB 03/06/18
MIT LL Nitrogen Vacancy Diamond Magnetometer
RF
initialization readoutOptical
Quantum System
NV– 13C, N, V
NV0
Quantum Engineering System Design
t
Engineer the quantum system and its environment through tailored diamond
growth
MIT LL grown diamond
3 m
m
Coherently control the quantum state to maximize field sensitivity
Machine learning algorithms search for optimized quantum
control
Optimize quantum system for neuron imaging
Quantum Sensing - 13DAB 03/06/18
Next Steps
Martinos Center Baseline with 302-Channel Conventional MEG
MIT LL Room Temperature Single SensorDemonstration
Diamond room-temperature demonstration coming soon
Quantum Sensing - 14DAB 03/06/18
Room Temperature MEG Contributors
Danielle BrajeLinh Pham
John BarryMike O’Keeffe
Chris McNallyErik Thompson
Jonah MajumderErik Eisenach
MIT LL Quantum Sensing Team:
Dirk Englund (MIT)
Ike Chuang (MIT)
Paola Capallero (MIT)
Phil Hemmer (Texas A&M)
Mark Newton and Gavin Morley (Warwick)
Matti Hämäläinen (Mass General Hospital)
Collaboration: