Electrodynamics and radiofrequency antenna concepts for human magnetic resonance at 23.5 T (1 GHz) and beyond.
← Research streamEMF simulations in phantoms and anatomical human head voxel models suggest that transmission fields suitable for 1H brain MR can be achieved at 1 GHz (23.5 T). Increasing transmit channel density around the head enhanced B1+ in the brain center. The calculate…
Study snapshot
Abstract
OBJECTIVE: This work investigates electrodynamic constraints, explores RF antenna concepts and examines the transmission fields (B 1 (+) ) and RF power deposition of dipole antenna arrays for (1)H magnetic resonance of the human brain at 1 GHz (23.5 T). MATERIALS AND METHODS: Electromagnetic field (EMF) simulations are performed in phantoms with average tissue simulants for dipole antennae using discrete frequencies [300 MHz (7.0 T) to 3 GHz (70.0 T)]. To advance to a human setup EMF simulations are conducted in anatomical human voxel models of the human head using a 20-element dipole array operating at 1 GHz. RESULTS: Our results demonstrate that transmission fields suitable for (1)H MR of the human brain can be achieved at 1 GHz. An increase in transmit channel density around the human head helps to enhance B 1 (+) in the center of the brain. The calculated relative increase in specific absorption rate at 23.5 versus 7.0 T was below 1.4 (in-phase phase setting) and 2.7 (circular polarized phase setting) for the dipole antennae array. CONCLUSION: The benefits of multi-channel dipole antennae at higher frequencies render MR at 23.5 T feasible from an electrodynamic standpoint. This very preliminary finding opens the door on further explorations that might be catalyzed into a 20-T class human MR system.
AI evidence extraction
Structured fields below were generated from the paper’s abstract and metadata to make the evidence easier to inspect. Automated extraction may be incomplete or incorrect; verify important details against the original paper.
Main findings
EMF simulations in phantoms and anatomical human head voxel models suggest that transmission fields suitable for 1H brain MR can be achieved at 1 GHz (23.5 T). Increasing transmit channel density around the head enhanced B1+ in the brain center. The calculated relative SAR increase at 23.5 T versus 7.0 T was below 1.4 (in-phase) and 2.7 (circular polarized) for the dipole array.
Outcomes measured
- Transmission fields (B1+)
- RF power deposition
- Specific absorption rate (SAR) (relative increase at 23.5 T vs 7.0 T)
Limitations
- Simulation-based study (EMF simulations in phantoms and voxel models)
- Described as a "very preliminary" finding
- SAR results reported as relative increase; absolute SAR not provided in abstract
View raw extracted JSON
{
"study_type": "engineering",
"exposure": {
"band": "RF",
"source": "MRI (human magnetic resonance) dipole antenna array",
"frequency_mhz": 1000,
"sar_wkg": null,
"duration": null
},
"population": null,
"sample_size": null,
"outcomes": [
"Transmission fields (B1+)",
"RF power deposition",
"Specific absorption rate (SAR) (relative increase at 23.5 T vs 7.0 T)"
],
"main_findings": "EMF simulations in phantoms and anatomical human head voxel models suggest that transmission fields suitable for 1H brain MR can be achieved at 1 GHz (23.5 T). Increasing transmit channel density around the head enhanced B1+ in the brain center. The calculated relative SAR increase at 23.5 T versus 7.0 T was below 1.4 (in-phase) and 2.7 (circular polarized) for the dipole array.",
"effect_direction": "unclear",
"limitations": [
"Simulation-based study (EMF simulations in phantoms and voxel models)",
"Described as a \"very preliminary\" finding",
"SAR results reported as relative increase; absolute SAR not provided in abstract"
],
"evidence_strength": "insufficient",
"confidence": 0.78,
"peer_reviewed_likely": "yes",
"keywords": [
"MRI",
"ultra-high field",
"23.5 T",
"1 GHz",
"dipole antenna array",
"B1+",
"RF power deposition",
"SAR",
"EMF simulations",
"human head voxel model",
"phantom"
],
"suggested_hubs": []
}AI-extracted fields are generated from the abstract and metadata and may be incomplete or incorrect. This material is for informational purposes and is not medical advice.
Identifiers and source
DOI: 10.1007/s10334-016-0559-y
PubMed: 27097905
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