Lucia Navarro de Lara

Dr. Lucia Navarro de Lara

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Research Focus & Metrics

Academic Career Length

13Years (2014-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 January 2021 in NeuroImage
Verified
Journal Article
Open access
LLLucia Navarro de Lara
Lucia Navarro de Lara
MDMohammad Daneshzand
Mohammad Daneshzand
AMAnthony Mascarenas
Anthony Mascarenas
DPDouglas Paulson
Douglas Paulson
KPKevin Pratt
Kevin Pratt
ANAapo Nummenmaa
Aapo Nummenmaa
Multichannel Transcranial Magnetic Stimulation (mTMS) arrays enable multiple sites to be stimulated simultaneously or sequentially under electronic control without moving the system’s stimulation coils. Here, we build and characterize the performance of a novel modular 3-axis TMS coil that can be utilized as a unit element in large-scale multichannel TMS arrays. We determined the basic physical characteristics of the 3-axis TMS coil x-, y- and z-elements using a custom 2-channel programmable stimulator prototype. We mapped the temporal rate-of-change of the induced magnetic field (dB/dt) on a 2D plane parallel to the coil surface (including an extended line for full spatial coverage) and compared those values with predictions from magnetic field simulations. Temperature measurements were carried out to assess the incorporated air-cooling method. We measured the mutual and self-inductances of the x/y/z-elements to assess coupling between them. Additionally, we measured and calculated the coupling between z-elements in the array configuration. Finally, we performed electric field simulations to evaluate the stimulation intensity and focality of the coil and compared the results to conventional TMS coils as well as demonstrated suitability of the 3-axis coil for a multichannel array configuration. The experimentally obtained dB/dt values validated the computational model of the 3-axis coil and therefore confirmed that both the coil and stimulator system are operating as intended. The air-cooling system was effective for brief high-frequency pulse trains and extended single- and paired-pulse TMS protocols. The electromagnetic simulations suggested that an array of the 3-axis coils would have comparable stimulation intensity to conventional TMS coils, therefore enabling clearly suprathreshold stimulation of the human brain. The recorded coil coupling between the x/y/z-elements was < 1% and the maximal coupling between z-elements in the array configuration was 1.8% and 3.4% for the measured and calculated values, respectively. We presented a 3-axis coil intended for multichannel TMS arrays. The electromagnetic measurements and simulations verified that the coil fabrication met the desired specifications and that the inductive coupling between the elements was negligible. The air-cooled 3-axis TMS coil appears suitable to be used as an element in multichannel TMS arrays.

24 November 2014 in Magnetic Resonance in Medicine
Verified
Journal Article
Open access
PDF file
LLLucia Navarro de Lara
Lucia Navarro de Lara
Christian WindischbergerChristian Windischberger
Christian Windischberger
Andre KuehneAndre Kuehne
Andre Kuehne
MWMichael Woletz
Michael Woletz
JSJürgen Sieg
Jürgen Sieg
ELElmar Laistler
Elmar Laistler
Purpose: To overcome current limitations in combined transcranial magnetic stimulation (TMS) and functional magnetic resonance imaging (fMRI) studies by employing a dedicated coil array design for 3 Tesla.Methods: The state‐of‐the‐art setup for concurrent TMS/fMRI is to use a large birdcage head coil, with the TMS between the subject's head and the MR coil. This setup has drawbacks in sensitivity, positioning, and available imaging techniques. In this study, an ultraslim 7‐channel receive‐only coil array for 3 T, which can be placed between the subject's head and the TMS, is presented. Interactions between the devices are investigated and the performance of the new setup is evaluated in comparison to the state‐of‐the‐art setup.Results: MR sensitivity obtained at the depth of the TMS stimulation is increased by a factor of five. Parallel imaging with an acceleration factor of two is feasible with low g‐factors. Possible interactions between TMS and the novel hardware were investigated and were found negligible.Conclusion: The novel coil array is safe, strongly improves signal‐to‐noise ratio in concurrent TMS/fMRI experiments, enables parallel imaging, and allows for flexible positioning of the TMS on the head while ensuring efficient TMS stimulation due to its ultraslim design. Magn Reson Med 74:1492–1501, 2015. © 2014 The Authors. Magnetic Resonance in Medicine published by Wiley Periodicals, Inc. on behalf of International Society for Magnetic Resonance in Medicine.

1 April 2017 in NeuroImage
Verified
Journal Article
Closed access
LLLucia Navarro de Lara
Lucia Navarro de Lara
MTMartin Tik
Martin Tik
MWMichael Woletz
Michael Woletz
RFRoberta Frass-Kriegl
Roberta Frass-Kriegl
EMEwald Moser
Ewald Moser
Christian WindischbergerChristian Windischberger
Christian Windischberger

1 August 2021 in NeuroImage
Verified
Journal Article
Open access
MDMohammad Daneshzand
Mohammad Daneshzand
SMSergey N. Makarov
Sergey N. Makarov
LLLucia Navarro de Lara
Lucia Navarro de Lara
BGBastien Guerin
Bastien Guerin
JMJennifer McNab
Jennifer McNab
ANAapo Nummenmaa
Aapo Nummenmaa
TMS neuronavigation with on-line display of the induced electric field (E-field) has the potential to improve quantitative targeting and dosing of stimulation, but present commercially available solutions are limited by simplified approximations. Developing a near real-time method for accurate approximation of TMS induced E-fields with subject-specific high-resolution surface-based head models that can be utilized for TMS navigation. Magnetic dipoles are placed on a closed surface enclosing an MRI-based head model of the subject to define a set of basis functions for the incident and total E-fields that define the subject's Magnetic Stimulation Profile (MSP). The near real-time speed is achieved by recognizing that the total E-field of the coil only depends on the incident E-field and the conductivity boundary geometry. The total E-field for any coil position can be obtained by matching the incident field of the stationary dipole basis set with the incident E-field of the moving coil and applying the same basis coefficients to the total E-field basis functions. Comparison of the MSP-based approximation with an established TMS solver shows great agreement in the E-field amplitude (relative maximum error around 5%) and the spatial distribution patterns (correlation >98%). Computation of the E-field took ~100 ms on a cortical surface mesh with 120k facets. The numerical accuracy and speed of the MSP approximation method make it well suited for a wide range of computational tasks including interactive planning, targeting, dosing, and visualization of the intracranial E-fields for near real-time guidance of coil positioning.

10 June 2023 in Brain Stimulation
Verified
Journal Article
Open access
LLLucia Navarro de Lara
Lucia Navarro de Lara
JSJason P. Stockmann
Jason P. Stockmann
QMQinglei Meng
Qinglei Meng
BKBoris Keil
Boris Keil
AMAzma Mareyam
Azma Mareyam
ANAapo Nummenmaa
Aapo Nummenmaa
Multichannel Transcranial Magnetic Stimulation (mTMS) [1] is a novel non-invasive brain stimulation technique allowing multiple sites to be stimulated simultaneously or sequentially under electronic control without movement of the coils. To enable simultaneous mTMS and MR imaging, we have designed and constructed a whole-head 28-channel receive-only RF coil at 3T. A helmet-shaped structure was designed considering a specific layout for a mTMS system with holes for positioning the TMS units next to the scalp. Diameter of the TMS units defined the diameter of RF loops. The placement of the preamplifiers was designed to minimize possible interactions and to allow straightforward positioning of the mTMS units around the RF coil. Interactions between TMS-MRI were analyzed for the whole-head system extending the results presented in previous publications [2]. Both SNR- and g-factors maps were obtained to compare the imaging performance of the coil with commercial head coils. Sensitivity losses for the RF elements containing TMS units show a well-defined spatial pattern. Simulations indicate that the losses are predominantly caused by eddy currents on the coil wire windings. The average SNR performance of the TMSMR 28-channel coil is about 66% and 86% of the SNR of the 32/20-channel head coil respectively. The g-factor values of the TMSMR 28-channel coil are similar to the 32-channel coil and significantly better than the 20-channel coil. We present the TMSMR 28-channel coil, a head RF coil array to be integrated with a multichannel 3-axisTMS coil system, a novel tool that will enable causal mapping of human brain function.

23 January 2020 in Magnetic Resonance in Medicine
Verified
Journal Article
Closed access
PDF file
LLLucia Navarro de Lara
Lucia Navarro de Lara
LGLaleh Golestanirad
Laleh Golestanirad
SMSergey N. Makarov
Sergey N. Makarov
JSJason P. Stockmann
Jason P. Stockmann
LWLawrence L. Wald
Lawrence L. Wald
ANAapo Nummenmaa
Aapo Nummenmaa