Ventricular B1+ perturbation at 7 T – real effect or measurement artifact?

The objective of this work was to explore the origin of local B₁⁺ perturbations in the ventricles measured at 7 T. The B₁⁺ field in the human brain was mapped using four different MRI techniques: dual refocusing echo acquisition mode (DREAM), actual flip‐angle imaging (AFI), saturated double‐angle method (SDAM) and Bloch–Siegert shift (BSS). Electromagnetic field simulations of B₁⁺ were performed in male and female subject models to assess the dependence of the B₁⁺ distribution on the dielectric properties of cerebrospinal fluid and subject anatomy. All four B₁⁺ mapping techniques, based on different B₁⁺ encoding mechanisms, show ‘residual’ structure of the ventricles, with a slightly enhanced B₁⁺ field in the ventricles. Electromagnetic field simulations indicate that this effect is real and arises from the strong contrast in electrical conductivity between cerebrospinal fluid and brain tissue. The simulated results were in good agreement with those obtained in three volunteers. Measured local B₁⁺ perturbations in the ventricles at 7 T can be partially explained by the high contrast in electrical conductivity between cerebrospinal fluid and white matter, in addition to effects related to the particular B₁⁺ measurement technique used. Copyright © 2014 John Wiley & Sons, Ltd.     

On‐resonance and off‐resonance continuous wave constant amplitude spin‐lock and T1ρ quantification in the presence of B1 and B0 inhomogeneities

Spin‐lock MRI is a valuable diagnostic imaging technology, as it can be used to probe the macromolecule environment of tissues. Quantitative T_1ρ imaging is one application of spin‐lock MRI that is reported to be promising for a number of clinical applications. Spin‐lock is often performed with a continuous RF wave at a constant RF amplitude either on resonance or off resonance. However, both on‐ and off‐resonance spin‐lock approaches are susceptible to B₁ and B₀ inhomogeneities, which results in image artifacts and quantification errors. In this work, we report a continuous wave constant amplitude spin‐lock approach that can achieve negligible image artifacts in the presence of B₁ and B₀ inhomogeneities for both on‐ and off‐resonance spin‐lock. Under the adiabatic condition, by setting the maximum B₁ amplitude of the adiabatic pulses equal to the B₁ amplitude of spin‐lock RF pulse, the spins are ensured to align along the effective field throughout the spin‐lock process. We show that this results in simultaneous compensation of B₁ and B₀ inhomogeneities for both on‐ and off‐resonance spin‐lock. The relaxation effect during the entire adiabatic half passage (AHP) and reverse AHP, and the stationary solution of the Bloch‐McConnell equation present at off‐resonance frequency offset, are considered in the revised relaxation model. We demonstrate that these factors create a direct current component to the conventional relaxation model. In contrast to the previously reported dual‐acquisition method, the revised relaxation model just requires one acquisition to perform quantification. The simulation, phantom, and in vivo experiments demonstrate that the proposed approach achieves superior image quality compared with the existing methods, and the revised relaxation model can perform T_1ρ quantification with one acquisition instead of two.     

Wideband Self‐Grounded Bow‐Tie Antenna for Thermal MR

The objective of this study was the design, implementation, evaluation and application of a compact wideband self‐grounded bow‐tie (SGBT) radiofrequency (RF) antenna building block that supports anatomical proton (¹H) MRI, fluorine (¹⁹F) MRI, MR thermometry and broadband thermal intervention integrated in a whole‐body 7.0 T system. Design considerations and optimizations were conducted with numerical electromagnetic field (EMF) simulations to facilitate a broadband thermal intervention frequency of the RF antenna building block. RF transmission (B₁⁺) field efficiency and specific absorption rate (SAR) were obtained in a phantom, and the thigh of human voxel models (Ella, Duke) for ¹H and ¹⁹F MRI at 7.0 T. B₁⁺ efficiency simulations were validated with actual flip‐angle imaging measurements. The feasibility of thermal intervention was examined by temperature simulations (f = 300, 400 and 500 MHz) in a phantom. The RF heating intervention (P_in = 100 W, t = 120 seconds) was validated experimentally using the proton resonance shift method and fiberoptic probes for temperature monitoring. The applicability of the SGBT RF antenna building block for in vivo ¹H and ¹⁹F MRI was demonstrated for the thigh and forearm of a healthy volunteer. The SGBT RF antenna building block facilitated ¹⁹F and ¹H MRI at 7.0 T as well as broadband thermal intervention (234‐561 MHz). For the thigh of the human voxel models, a B₁⁺ efficiency ≥11.8 μT/√kW was achieved at a depth of 50 mm. Temperature simulations and heating experiments in a phantom demonstrated a temperature increase ΔT >7 K at a depth of 10 mm. The compact SGBT antenna building block provides technology for the design of integrated high‐density RF applicators and for the study of the role of temperature in (patho‐) physiological processes by adding a thermal intervention dimension to an MRI device (Thermal MR).     

Ultra‐high‐field RF coil development for evaluating upper extremity imaging applications

The purpose of this study is to develop and evaluate a custom‐designed 7  T MRI coil and explore its use for upper extremity applications. An RF system composed of a transverse electromagnetic transmit coil and an eight‐channel receive‐only array was developed for 7  T upper extremity applications. The RF system was characterized and evaluated using scattering parameters and B₁⁺ mapping. Finite difference time domain simulations were performed to evaluate the B₁⁺ field distribution and specific absorption rate for the forearm region of the upper extremity. High‐resolution 7  T images were acquired and compared with those at 3 T. The simulation and experimental results show very good B₁⁺ field homogeneity across the forearm. High‐resolution images of musculotendinous, osseocartilaginous, and neurovascular structures in the upper extremity are presented with T₁ volumetric interpolated breath‐hold examination, T₂ double‐echo steady state, T₂* susceptibility weighted imaging (SWI), diffusion tensor imaging, and time‐of‐flight sequences. Comparison between 3  T and 7  T is shown. Intricate contextual anatomy can be delineated in synovial, fibrocartilaginous, interosseous, and intraosseous trabecular structures of the forearm, as well as palmar and digital vascular anatomy (including microvascular detail in SWI). Ultra‐high‐field 7  T imaging holds great potential in improving the sensitivity and specificity of upper extremity imaging, especially in wrist and hand pathology secondary to bone, ligament, nerve, vascular, and other soft or hard tissue etiology.     

Estimating B1+ in the breast at 7 T using a generic template

Dynamic contrast‐enhanced MRI is the workhorse of breast MRI, where the diagnosis of lesions is largely based on the enhancement curve shape. However, this curve shape is biased by RF transmit (B₁⁺) field inhomogeneities. B₁⁺ field information is required in order to correct these. The use of a generic, coil‐specific B₁⁺ template is proposed and tested. Finite‐difference time‐domain simulations for B₁⁺ were performed for healthy female volunteers with a wide range of breast anatomies. A generic B₁⁺ template was constructed by averaging simulations based on four volunteers. Three‐dimensional B₁⁺ maps were acquired in 15 other volunteers. Root mean square error (RMSE) metrics were calculated between individual simulations and the template, and between individual measurements and the template. The agreement between the proposed template approach and a B₁⁺ mapping method was compared against the agreement between acquisition and reacquisition using the same mapping protocol. RMSE values (% of nominal flip angle) comparing individual simulations with the template were in the range 2.00‐4.01%, with mean 2.68%. RMSE values comparing individual measurements with the template were in the range8.1‐16%, with mean 11.7%. The agreement between the proposed template approach and a B₁⁺ mapping method was only slightly worse than the agreement between two consecutive acquisitions using the same mapping protocol in one volunteer: the range of agreement increased from ±16% of the nominal angle for repeated measurement to ±22% for the B₁⁺ template. With local RF transmit coils, intersubject differences in B₁⁺ fields of the breast are comparable to the accuracy of B₁⁺ mapping methods, even at 7 T. Consequently, a single generic B₁⁺ template suits subjects over a wide range of breast anatomies, eliminating the need for a time‐consuming B₁⁺ mapping protocol.     

On the transmit field inhomogeneity correction of relaxation‐compensated amide and NOE CEST effects at 7 T

High field MRI is beneficial for chemical exchange saturation transfer (CEST) in terms of high SNR, CNR, and chemical shift dispersion. These advantages may, however, be counter‐balanced by the increased transmit field inhomogeneity normally associated with high field MRI. The relatively high sensitivity of the CEST contrast to B₁ inhomogeneity necessitates the development of correction methods, which is essential for the clinical translation of CEST. In this work, two B₁ correction algorithms for the most studied CEST effects, amide‐CEST and nuclear Overhauser enhancement (NOE), were analyzed. Both methods rely on fitting the multi‐pool Bloch‐McConnell equations to the densely sampled CEST spectra. In the first method, the correction is achieved by using a linear B₁ correction of the calculated amide and NOE CEST effects. The second method uses the Bloch‐McConnell fit parameters and the desired B₁ amplitude to recalculate the CEST spectra, followed by the calculation of B₁‐corrected amide and NOE CEST effects. Both algorithms were systematically studied in Bloch‐McConnell equations and in human data, and compared with the earlier proposed ideal interpolation‐based B₁ correction method. In the low B₁ regime of 0.15–0.50 μT (average power), a simple linear model was sufficient to mitigate B₁ inhomogeneity effects on a par with the interpolation B₁ correction, as demonstrated by a reduced correlation of the CEST contrast with B₁ in both the simulations and the experiments.     

Non‐invasive temperature mapping using temperature‐responsive water saturation shift referencing (T‐WASSR) MRI

We present a non‐invasive MRI approach for assessing the water proton resonance frequency (PRF) shifts associated with changes in temperature. This method is based on water saturation shift referencing (WASSR), a method first developed for assessing B₀ field inhomogeneity. Temperature‐induced water PRF shifts were determined by estimating the frequency of the minimum intensity of the water direct saturation spectrum at each temperature using Lorentzian line‐shape fitting. The change in temperature was then calculated from the difference in water PRF shifts between temperatures. Optimal acquisition parameters were first estimated using simulations and later confirmed experimentally. Results in vitro and in vivo showed that the temperature changes measured using the temperature‐responsive WASSR (T‐WASSR) were in good agreement with those obtained with MR spectroscopy or phase‐mapping‐based water PRF measurement methods,. In addition, the feasibility of temperature mapping in fat‐containing tissue is demonstrated in vitro. In conclusion, the T‐WASSR approach provides an alternative for non‐invasive temperature mapping by MRI, especially suitable for temperature measurements in fat‐containing tissues. Copyright © 2014 John Wiley & Sons, Ltd.     

B0 inhomogeneity‐insensitive triple‐quantum‐filtered sodium imaging using a 12‐step phase‐cycling scheme

Triple‐quantum‐filtered (TQF) sodium MRI can be used to separate sodium NMR signals from different physiological compartments. Although three‐pulse triple‐quantum filtering has been demonstrated to be better suited for in vivo imaging, the absence of the refocusing pulse in the filter increases its sensitivity to magnetic field inhomogeneities. Therefore, several TQF cycles have been developed previously to correct image distortions caused by B₀ inhomogeneities. In this paper, we present a new 12‐step phase‐cycling TQF scheme based on three radiofrequency pulses which allows the compensation of B₀ variations both with and without ancillary B₀ map information. The method offers 40% higher signal‐to‐noise‐ratio efficiency compared with the previously developed B₀‐correcting phase‐cycling schemes. Copyright © 2010 John Wiley & Sons, Ltd.     

Small‐animal,whole‐body imaging with metamaterial‐inspired RF coil

Particular applications in preclinical magnetic resonance imaging require the entire body of an animal to be imaged with sufficient quality. This is usually performed by combining regions scanned with small coils with high sensitivity or long scans using large coils with low sensitivity. Here, a metamaterial‐inspired design employing a parallel array of wires operating on the principle of eigenmode hybridization was used to produce a small‐animal imaging coil. The coil field distribution responsible for the coil field of view and sensitivity was simulated in an electromagnetic simulation package and the coil geometrical parameters were optimized for whole‐body imaging. A prototype coil was then manufactured and assembled using brass telescopic tubes with copper plates as distributed capacitance. Its field distribution was measured experimentally using the B₁⁺ mapping technique and was found to be in close correspondence with the simulated results. The coil field distribution was found to be suitable for large field of view small‐animal imaging and the coil image quality was compared with a commercially available coil by whole‐body scanning of living mice. Signal‐to‐noise measurements in living mice showed higher values than those of a commercially available coil with large receptive fields, and rivalled the performance of small receptive field and high‐sensitivity coils. The coil was deemed to be suitable for some whole‐body, small‐animal preclinical applications.     

Extended RF shimming: Sequence‐level parallel transmission optimization applied to steady‐state free precession MRI of the heart

Cardiac magnetic resonance imaging (MRI) at high field presents challenges because of the high specific absorption rate and significant transmit field (B₁⁺) inhomogeneities. Parallel transmission MRI offers the ability to correct for both issues at the level of individual radiofrequency (RF) pulses, but must operate within strict hardware and safety constraints. The constraints are themselves affected by sequence parameters, such as the RF pulse duration and TR, meaning that an overall optimal operating point exists for a given sequence. This work seeks to obtain optimal performance by performing a ‘sequence‐level’ optimization in which pulse sequence parameters are included as part of an RF shimming calculation. The method is applied to balanced steady‐state free precession cardiac MRI with the objective of minimizing TR, hence reducing the imaging duration. Results are demonstrated using an eight‐channel parallel transmit system operating at 3 T, with an in vivo study carried out on seven male subjects of varying body mass index (BMI). Compared with single‐channel operation, a mean‐squared‐error shimming approach leads to reduced imaging durations of 32 ± 3% with simultaneous improvement in flip angle homogeneity of 32 ± 8% within the myocardium.     

Improved off‐resonance phase behavior using a phase‐inverted adiabatic half‐passage pulse for 13C MRS in humans at 7 T

In vivo ¹³C MRS at high field benefits from an improved SNR and spectral resolution especially when using surface coils in combination with adiabatic pulses, such as the adiabatic half‐passage (AHP) pulse for ¹³C excitation. However, the excitation profile of the AHP pulse is asymmetric relative to the carrier frequency, which could lead to asymmetric excitation of the spectral lines relative to the center of the spectrum. In this study, a pulse‐acquire sequence was designed for adiabatic ¹³C excitation with a symmetric bandwidth, utilizing a combination of two AHP pulses with inverted phases in alternate scans. Magnetization and phase behavior as a function of frequency offset and RF amplitude of the B₁ field, as well as the steady‐state transverse magnetization response to off‐resonance, were simulated. Excitation properties of the combined pulse sequence were studied by ²³Na imaging and ¹³C spectroscopy in vitro on a phantom and in vivo on the human calf at 7 T. Simulations demonstrated symmetric transverse magnetization and phase with respect to positive and negative frequency offsets when using two AHP pulses with inverted phases in alternate scans, thereby minimizing baseline distortion and achieving symmetric T₁ weighting, as confirmed by in vitro measurements. The intensities of the lipid peaks at 15, 30, 62, 73, and 130 ppm were in agreement with those theoretically predicted using two AHP pulses with inverted phases in alternate scans. We conclude that using two phase‐inverted AHP pulses improves the symmetry of the ¹³C excitation profile and phase response to off‐resonance effects at 7 T in comparison with using a single AHP pulse.     

High‐permittivity solid ceramic resonators for high‐field human MRI

The properties of a ceramic‐based annular dielectric resonator designed for 7 T MRI have been examined. Electromagnetic simulations and experimentally determined modal frequencies agree to within ~1%. The dependence of the resonance frequency of the degenerate quadrature HEM₁₁ modes on hole diameter and shield diameter was also investigated. The constructed coil, with a 2.5 cm diameter hole, had an unloaded Q value of 400, which was reduced to 150 when loaded with a human finger. Simulated and experimental B₁⁺ maps show a high degree of homogeneity with a sensitivity of ~11.5 μT/√W at the centre. A comparison with a loop gap resonator showed an approximately 25% higher sensitivity for the dielectric resonator. High‐resolution images of the digital interphalangeal (DIP) and proximal interphalangeal (PIP) joints of volunteers were acquired in imaging times of less than 2 min. Finally, novel methods of double tuning such ceramic resonators to two relatively close frequencies, e.g. proton and fluorine, have been shown. Copyright © 2013 John Wiley & Sons, Ltd.     

Slice‐selective FID acquisition,localized by outer volume suppression (FIDLOVS) for 1H‐MRSI of the human brain at 7 T with minimal signal loss

In comparison to 1.5 and 3 T, MR spectroscopic imaging at 7 T benefits from signal‐to‐noise ratio (SNR) gain and increased spectral resolution and should enable mapping of a large number of metabolites at high spatial resolutions. However, to take full advantage of the ultra‐high field strength, severe technical challenges, e.g. related to very short T₂ relaxation times and strict limitations on the maximum achievable B₁ field strength, have to be resolved. The latter results in a considerable decrease in bandwidth for conventional amplitude modulated radio frequency pulses (RF‐pulses) and thus to an undesirably large chemical‐shift displacement artefact. Frequency‐modulated RF‐pulses can overcome this problem; but to achieve a sufficient bandwidth, long pulse durations are required that lead to undesirably long echo‐times in the presence of short T₂ relaxation times. In this work, a new magnetic resonance spectroscopic imaging (MRSI) localization scheme (free induction decay acquisition localized by outer volume suppression, FIDLOVS) is introduced that enables MRSI data acquisition with minimal SNR loss due to T₂ relaxation and thus for the first time mapping of an extended neurochemical profile in the human brain at 7 T. To overcome the contradictory problems of short T₂ relaxation times and long pulse durations, the free induction decay (FID) is directly acquired after slice‐selective excitation. Localization in the second and third dimension and skull lipid suppression are based on a T₁‐ and B₁‐insensitive outer volume suppression (OVS) sequence. Broadband frequency‐modulated excitation and saturation pulses enable a minimization of the chemical‐shift displacement artefact in the presence of strict limits on the maximum B₁ field strength. The variable power RF pulses with optimized relaxation delays (VAPOR) water suppression scheme, which is interleaved with OVS pulses, eliminates modulation side bands and strong baseline distortions. Third order shimming is based on the accelerated projection‐based automatic shimming routine (FASTERMAP) algorithm. The striking SNR and spectral resolution enable unambiguous quantification and mapping of 12 metabolites including glutamate (Glu), glutamine (Gln), N‐acetyl‐aspartatyl‐glutamate (NAAG), γ‐aminobutyric acid (GABA) and glutathione (GSH). The high SNR is also the basis for highly spatially resolved metabolite mapping. Copyright © 2009 John Wiley & Sons, Ltd.     

Triple‐echo steady‐state T2 relaxometry of the human brain at high to ultra‐high fields

Quantitative MRI techniques, such as T₂ relaxometry, have demonstrated the potential to detect changes in the tissue microstructure of the human brain with higher specificity to the underlying pathology than in conventional morphological imaging. At high to ultra‐high field strengths, quantitative MR‐based tissue characterization benefits from the higher signal‐to‐noise ratio traded for either improved resolution or reduced scan time, but is impaired by severe static (B₀) and transmit (B₁) field heterogeneities. The objective of this study was to derive a robust relaxometry technique for fast T₂ mapping of the human brain at high to ultra‐high fields, which is highly insensitive to B₀ and B₁ field variations. The proposed method relies on a recently presented three‐dimensional (3D) triple‐echo steady‐state (TESS) imaging approach that has proven to be suitable for fast intrinsically B₁‐insensitive T₂ relaxometry of rigid targets. In this work, 3D TESS imaging is adapted for rapid high‐ to ultra‐high‐field two‐dimensional (2D) acquisitions. The achieved short scan times of 2D TESS measurements reduce motion sensitivity and make TESS‐based T₂ quantification feasible in the brain. After validation in vitro and in vivo at 3 T, T₂ maps of the human brain were obtained at 7 and 9.4 T. Excellent agreement between TESS‐based T₂ measurements and reference single‐echo spin‐echo data was found in vitro and in vivo at 3 T, and T₂ relaxometry based on TESS imaging was proven to be feasible and reliable in the human brain at 7 and 9.4 T. Although prominent B₀ and B₁ field variations occur at ultra‐high fields, the T₂ maps obtained show no B₀‐ or B₁‐related degradations. In conclusion, as a result of the observed robustness, TESS T₂ may emerge as a valuable measure for the early diagnosis and progression monitoring of brain diseases in high‐resolution 2D acquisitions at high to ultra‐high fields. Copyright © 2014 John Wiley & Sons, Ltd.     

Development of a 7 T RF coil system for breast imaging

In ultrahigh‐field MRI, such as 7 T, the signal‐to‐noise ratio (SNR) increases while transmit (Tx) field (B₁⁺) can be degraded due to inhomogeneity and elevated specific absorption rate (SAR). By applying new array coil concepts to both Tx and receive (Rx) coils, the B₁⁺ homogeneity and SNR can be improved. In this study, we developed and tested in vivo a new RF coil system for 7 T breast MRI. An RF coil system composed of an eight‐channel Tx‐only array based on a tic‐tac‐toe design (can be combined to operate in single‐Tx mode) in conjunction with an eight‐channel Rx‐only insert was developed. Characterizations of the B₁⁺ field and associated SAR generated by the developed RF coil system were numerically calculated and empirically measured using an anatomically detailed breast model, phantom and human breasts. In vivo comparisons between 3 T (using standard commercial solutions) and 7 T (using the newly developed coil system) breast imaging were made. At 7 T, about 20% B₁⁺ inhomogeneity (standard deviation over the mean) was measured within the breast tissue for both the RF simulations and 7 T experiments. The addition of the Rx‐only array enhances the SNR by a factor of about three. High‐quality MR images of human breast were acquired in vivo at 7 T. For the in vivo comparisons between 3 T and 7 T, an approximately fourfold increase of SNR was measured with 7 T imaging. The B₁⁺ field distributions in the breast model, phantom and in vivo were in reasonable agreement. High‐quality 7 T in vivo breast MRI was successfully acquired at 0.6 mm isotropic resolution using the newly developed RF coil system.     

19 F MRSI of capecitabine in the liver at 7 T using broadband transmit–receive antennas and dual‐band RF pulses

Capecitabine (Cap) is an often prescribed chemotherapeutic agent, successfully used to cure some patients from cancer or reduce tumor burden for palliative care. However, the efficacy of the drug is limited, it is not known in advance who will respond to the drug and it can come with severe toxicity. ¹⁹ F Magnetic Resonance Spectroscopy (MRS) and Magnetic Resonance Spectroscopic Imaging (MRSI) have been used to non‐invasively study Cap metabolism in vivo to find a marker for personalized treatment. In vivo detection, however, is hampered by low concentrations and the use of radiofrequency (RF) surface coils limiting spatial coverage. In this work, the use of a 7T MR system with radiative multi‐channel transmit–receive antennas was investigated with the aim of maximizing the sensitivity and spatial coverage of ¹⁹ F detection protocols. The antennas were broadband optimized to facilitate both the ¹H (298 MHz) and ¹⁹ F (280 MHz) frequencies for accurate shimming, imaging and signal combination. B₁⁺ simulations, phantom and noise measurements showed that more than 90% of the theoretical maximum sensitivity could be obtained when using B₁⁺ and B₁^? information provided at the ¹H frequency for the optimization of B₁⁺ and B₁^? at the ¹⁹ F frequency. Furthermore, to overcome the limits in maximum available RF power, whilst ensuring simultaneous excitation of all detectable conversion products of Cap, a dual‐band RF pulse was designed and evaluated. Finally, ¹⁹ F MRS(I) measurements were performed to detect ¹⁹ F metabolites in vitro and in vivo. In two patients, at 10 h (patient 1) and 1 h (patient 2) after Cap intake, ¹⁹ F metabolites were detected in the liver and the surrounding organs, illustrating the potential of the set‐up for in vivo detection of metabolic rates and drug distribution in the body. Copyright © 2015 John Wiley & Sons, Ltd.     

Advantages of chemical exchange‐sensitive spin‐lock (CESL) over chemical exchange saturation transfer (CEST) for hydroxyl– and amine–water proton exchange studies

The chemical exchange (CE) rate of endogenous hydroxyl and amine protons with water is often comparable to the difference in their chemical shifts. These intermediate exchange processes have been imaged by the CE saturation transfer (CEST) approach with low‐power and long‐duration irradiation. However, the sensitivity is not optimal and, more importantly, the signal is contaminated by slow magnetization transfer processes. Here, the properties of CEST signals are compared with those of a CE‐sensitive spin‐lock (CESL) technique irradiating at the labile proton frequency. First, using a higher power and shorter irradiation in CE‐MRI, we obtain: (i) an increased selectivity to faster CE rates via a higher sensitivity to faster CEs and a lower sensitivity to slower CEs and magnetization transfer processes; and (ii) a decreased in vivo asymmetric magnetization transfer contrast measured at ±15 ppm. The sensitivity gain of CESL over CEST is higher for a higher power and shorter irradiation. Unlike CESL, CEST signals oscillate at a very high power and short irradiation. Second, time‐dependent CEST and CESL signals are well modeled by analytical solutions of CE‐MRI with an asymmetric population approximation, which can be used for quantitative CE‐MRI and validated by simulations of Bloch–McConnell equations and phantom experiments. Finally, the in vivo amine–water proton exchange contrast measured at 2.5 ppm with ω₁ = 500 Hz is 18% higher in sensitivity for CESL than CEST at 9.4 T. Overall, CESL provides better exchange rate selectivity and sensitivity than CEST; therefore, CESL is more suitable for CE‐MRI of intermediate exchange protons. Copyright © 2014 John Wiley & Sons, Ltd.     

Exchange‐dependent relaxation in the rotating frame for slow and intermediate exchange – modeling off‐resonant spin‐lock and chemical exchange saturation transfer

Chemical exchange observed by NMR saturation transfer (CEST) and spin‐lock (SL) experiments provide an MRI contrast by indirect detection of exchanging protons. The determination of the relative concentrations and exchange rates is commonly achieved by numerical integration of the Bloch–McConnell equations. We derive an analytical solution of the Bloch–McConnell equations that describes the magnetization of coupled spin populations under radiofrequency irradiation. As CEST and off‐resonant SL are equivalent, their steady‐state magnetization and dynamics can be predicted by the same single eigenvalue: the longitudinal relaxation rate in the rotating frame R_1ρ. For the case of slowly exchanging systems, e.g. amide protons, the saturation of the small proton pool is affected by transverse relaxation (R_2b). It turns out, that R_2b is also significant for intermediate exchange, such as amine‐ or hydroxyl‐exchange or paramagnetic CEST agents, if pools are only partially saturated. We propose a solution for R_1ρ that includes R₂ of the exchanging pool by extending existing approaches, and verify it by numerical simulations. With the appropriate projection factors, we obtain an analytical solution for CEST and SL for nonzero R₂ of the exchanging pool, exchange rates in the range 1–10⁴ Hz, B₁ from 0.1 to 20 μT and arbitrary chemical shift differences between the exchanging pools, whilst considering the dilution by direct water saturation across the entire Z‐spectra. This allows the optimization of irradiation parameters and the quantification of pH‐dependent exchange rates and metabolite concentrations. In addition, we propose evaluation methods that correct for concomitant direct saturation effects. It is shown that existing theoretical treatments for CEST are special cases of this approach. Copyright © 2012 John Wiley & Sons, Ltd.     

Image‐guided radio‐frequency gain calibration for high‐field MRI

High‐field (≥ 3T) MRI provides a means to increase the signal‐to‐noise ratio, due to its higher tissue magnetization compared with 1.5T. However, both the static magnetic field (B₀) and the transmit radio‐frequency (RF) field (B) inhomogeneities are comparatively higher at higher field strengths than those at 1.5T. These challenging factors at high‐field strengths make it more difficult to accurately calibrate the transmit RF gain using standard RF calibration procedures. An image‐based RF calibration procedure was therefore developed, in order to accurately calibrate the transmit RF gain within a specific region‐of‐interest (ROI). Using a turbo fast low‐angle shot (TurboFLASH) pulse sequence with centric k‐space reordering, a series of ‘saturation‐no‐recovery’ images was acquired by varying the flip angle of the preconditioning pulse. In the resulting images, the signal null occurs in regions where the flip angle of the preconditioning pulse is 90°. For a given ROI, the mean signal can be plotted as a function of the nominal flip angle, and the resulting curve can be used to quantitatively identify the signal null. This image‐guided RF calibration procedure was evaluated through phantom and volunteer imaging experiments at 3T and 7T. The image‐guided RF calibration results in vitro were consistent with standard B₀ and B maps. The standard automated RF calibration procedure produced approximately 20% and 15–30% relative error in the transmit RF gain in the left kidney at 3T and brain at 7T, respectively. For initial application, a T₂ mapping pulse sequence was applied at 7T. The T₂ measurements in the thalamus at 7T were 60.6 ms and 48.2 ms using the standard and image‐guided RF calibration procedures, respectively. This rapid, image‐guided RF calibration procedure can be used to optimally calibrate the flip angle for a given ROI and thus minimize measurement errors for quantitative MRI and MR spectroscopy. Copyright © 2009 John Wiley & Sons, Ltd.     

Comparison of spoiled gradient echo and steady‐state free‐precession imaging for native myocardial T1 mapping using the slice‐interleaved T1 mapping (STONE) sequence

Cardiac T₁ mapping allows non‐invasive imaging of interstitial diffuse fibrosis. Myocardial T₁ is commonly calculated by voxel‐wise fitting of the images acquired using balanced steady‐state free precession (SSFP) after an inversion pulse. However, SSFP imaging is sensitive to B₁ and B₀ imperfection, which may result in additional artifacts. A gradient echo (GRE) imaging sequence has been used for myocardial T₁ mapping; however, its use has been limited to higher magnetic field to compensate for the lower signal‐to‐noise ratio (SNR) of GRE versus SSFP imaging. A slice‐interleaved T₁ mapping (STONE) sequence with SSFP readout (STONE–SSFP) has been recently proposed for native myocardial T₁ mapping, which allows longer recovery of magnetization (>8 R–R) after each inversion pulse. In this study, we hypothesize that a longer recovery allows higher SNR and enables native myocardial T₁ mapping using STONE with GRE imaging readout (STONE–GRE) at 1.5T. Numerical simulations and phantom and in vivo imaging were performed to compare the performance of STONE–GRE and STONE–SSFP for native myocardial T₁ mapping at 1.5T. In numerical simulations, STONE–SSFP shows sensitivity to both T₂ and off resonance. Despite the insensitivity of GRE imaging to T₂, STONE–GRE remains sensitive to T₂ due to the dependence of the inversion pulse performance on T₂. In the phantom study, STONE–GRE had inferior accuracy and precision and similar repeatability as compared with STONE–SSFP. In in vivo studies, STONE–GRE and STONE–SSFP had similar myocardial native T₁ times, precisions, repeatabilities and subjective T₁ map qualities. Despite the lower SNR of the GRE imaging readout compared with SSFP, STONE–GRE provides similar native myocardial T₁ measurements, precision, repeatability, and subjective image quality when compared with STONE–SSFP at 1.5T.