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An optical‐based active detuning for single and dual channel/loop endoluminal surface coils

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An optical-based active detuning for single and dual channel/loop endoluminal surface coils

Isabelle Saniour, Anne-Laure Perrier, Lionel Duvillaret, Raphaël Sablong, Gwenaël Gaborit, Olivier Beuf

To cite this version:

Isabelle Saniour, Anne-Laure Perrier, Lionel Duvillaret, Raphaël Sablong, Gwenaël Gaborit, et al.. An

optical-based active detuning for single and dual channel/loop endoluminal surface coils. ESMRMB

2017 CONGRESS, Oct 2017, Barcelona, Spain. �hal-01693614�

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5) Yarnykh, MRM 2007;57:192.

6) Lattanzi R et al., MRM 2012;68:286.

7) Pfrommer A et al., Proc.ISMRM 24,2016,175.

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An optical-based active detuning for single and dual channel/loop endoluminal surface coils

I. Saniour1, A.-L. Perrier2, L. Duvillaret3, R. Sablong1, G. Gaborit2, O. Beuf1

1CREATIS, Univ. Lyon; CNRS UMR 5220; INSERM U1206; INSA- Lyon; UJM-Saint Etienne; Universite´ Lyon1, Villeurbanne/FRANCE,

2IMEP-LAHC, Univ. Savoie-Mont-Blanc, Le Bourget-du-Lac/

FRANCE,3kapteos, Kapteos, Sainte-He´le`ne-du-Lac/FRANCE

Purpose/Introduction: Sub-centimeter endoluminal receiver coils dedicated to MRI are the best candidates for early depiction of colonic diseases1,2. Nevertheless, the clinical use of these coils is controver- sial because the impossibility of using devices such as RF traps can cause strong local heating3. Besides, the sensitivity of a single-loop coil is orientation-dependent with respect to the magnetic field4. Our overall objective is to develop a fully-optical multichannel endolu- minal coil ensuring patient safety while achieving high signal-to- noise ratio (SNR) and better radial uniformity5. Optical transmission of the NMR signal6combining active optical detuning7could be a secure alternative solution. Here we present an optical-based circuit for simultaneous detuning of two channels/loops endoluminal coil.

Subjects and Methods:A dual-channel/loop (DCL) endoluminal coil was built; it consists of two independent rectangular loops associated to a single active detuning circuit. The loops (resonant circuit) were realized according to previous works2,7and were geometrically ori- ented in quadrature. Optical detuning was carried out using two photodiodes that generate a DC current when illuminated thus acti- vating the PIN diodes placed in parallel to each loop. The performances of this coil were compared to a reference coil having the same resonant circuit but using a galvanic connection to transmit the DC current for PIN diode activation (classic detuning). Besides, two single-loop coils were built with optical and classic detuning circuits, respectively. Figure 1 illustrates the electronic schematic of the different coils. For DCL coils, the S-parameters were studied to assess the detuning performances and the mutual coupling between the loops (for DCL coils). Finally, these coils were inserted into a cylindrical phantom to acquire MR images in a 3T MRI.

Results: At the resonance frequency, the |S21|-parameters were around-24.86 and-30 dB respectively for the optical and classic detuning DCL coils (Fig. 2). Figure 3 shows that the signal distri- bution and SNR of images taken by a DCL coil were enhanced compared to single-loop coil images. Finally, MR images of optical detuned coils are very much comparable to those with classic detuned coils.

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Discussion/Conclusion: On the experimental bench, the |S21|-pa- rameter proves that the two loops are geometrically decoupled and independent.

MR images verify that active optical detuning is effective and the generated current was sufficient to detune simultaneously the two loops that cannot be used separately in this particular case (Fig. 1a).

The concept of this optical detuning circuit could be implemented whatever the geometry of the coils and the number of channels.

References:

1. Geenen RWF, Hussain SM, Siersema PD, Poley JW, Kuipers E J and KrestinGP 2007 Current status of MRI in patients with inflam- matory bowel disease colitisAppl. Radiol.3610–22

2. Beuf O, Pilleul F, Armenean M, Hadour G and Saint-Jalmes H 2004 In vivo colon wall imaging using endoluminal coils: feasibility study on rabbitsJ. Magn. Reson. Imaging2090–6

3. Detti V, Grenier D, Perrin E and BeufO2011 Assessment of radiofrequency self-heating around a metallic wire with MR T1-based thermometry Magn. Reson. Med.66448–55

4. Beuf O, Armenean M, Pilleul F and Saint-Jalmes H 2002 Signal distribution with endoluminal loop radiofrequency coils: effect of orientation in the magnetic field Proc. ESMRMB

5. Hoult D I, Chen C N and Sank V J 1983 Quadrature detection in the Laboratory frame.J. Magn. Reson. Med.54339–53

6. Ayde´ A, Gaborit G, Dahdah J, Duvillaret L, Courjal N, Guyot C, Sablong R, Perrier A L and Beuf O 2014 Unbiased electrooptic waveguide as a sensitive nuclear magnetic resonance sensorIEEE Photonics Technol. Lett.261266–9

7. Saniour I, Ayde´ A, Perrier AL, Gaborit G, Duvillaret L, Sablong R and Beuf O Active optical-based detuning circuit for receiver endo- luminal coil 2017Biomedical Physics & Engineering Express31–10 Acknowledgements

Authors thank Dr Simon Lambert for advices in building the coil and Auvergne-Rhoˆne-Alpes region, DGA and LabEX PRIMES (ANR-11- IDEX-0007) for financial support.

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A Flexible Transceiver Array for 7 T Cardiac MRI:

First Imaging Experiments

S. Hosseinnezhadian1, R. Frass-Kriegl1, S. Goluch1, M. Pichler1, J. Sieg1, M. Poirier-Quinot2, L. Darrasse2, E. Moser1, J.-C. Ginefri2, E. Laistler1

1Division MR Physics - Center for Medical Physics and Biomedical Engineering, Medical University of Vienna, Vienna/AUSTRIA,2IR4M (Imagerie par Re´sonance Magne´tique Me´dicale et Multi-modalite´s), Univ. Paris-Sud, CNRS, UMR8081, Universite´ Paris-Saclay, Orsay/

FRANCE

Purpose/Introduction:Mechanically flexible arrays of transmission line resonators (TLRs) combine the advantages of parallel imaging with the possibility of form-fitting [1]. Mutual decoupling of the individual elements is one of the major technical challenges in designing TLR arrays. A decoupling ring-based technique [2] has been shown to be efficient [3]. In this work, we demonstrate the performance of a 12-element TLR flexible array with decoupling rings in bench tests and MR measurements at 7T.

Subjects and Methods: Figure 1a, c shows the schematic of the single element TLR and the 12-element TLR array with overlapped decoupling rings. The overlap distance was optimized analytically to minimize the shared magnetic flux [4]. Initially, the performance of the 12-element array was evaluated in 3D EMS (XFdtd 7.5, Remcom, USA) and circuit co-simulation [5] (ADS, Keysight Technologies, USA) by simulating scattering parameters and electromagnetic fields [3]. Fabrication of the flexible PCB was outsourced.

The transmit power was split among elements according to the dia- gram shown in Fig. 1bc. A static phase shimming algorithm [6] was used to optimize B1+ efficiency and homogeneity in a ROI. Phases between columns of elements were varied, while phases between elements within one column were kept equal. The determined phase configuration was implemented using cables with different lengths.

MRI experiments were conducted on a 7T whole body MRI scanner (Siemens Healthcare, Erlangen, Germany). Flip angle maps were acquired using the Saturated Turbo FLASH method [7], applying a slice-selective saturation pulse (2 ms duration, 50 V amplitude). B1+ maps normalized to the input power were calculated using measured flip angle maps considering the losses from cabling, interface board, and reflection due to imperfect matching on the phantom, because matching had been adjusted for an average human torso. MR images of a box-shaped phantom were acquired with the array in flat configuration.

Results:Figure 2a shows simulated and measured scattering param- eters, demonstrating efficient matching and decoupling for all

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