Oxygen‐dependent hyperpolarized 129Xe brain MR

Hyperpolarized (HP) ¹²⁹Xe MR offers unique advantages for brain functional imaging (fMRI) because of its extremely high sensitivity to different chemical environments and the total absence of background noise in biological tissues. However, its advancement and applications are currently plagued by issues of signal strength. Generally, xenon atoms found in the brain after inhalation are transferred from the lung via the bloodstream. The longitudinal relaxation time (T₁) of HP ¹²⁹Xe is inversely proportional to the pulmonary oxygen concentration in the lung because oxygen molecules are paramagnetic. However, the T₁ of ¹²⁹Xe is proportional to the pulmonary oxygen concentration in the blood, because the higher pulmonary oxygen concentration will result in a higher concentration of diamagnetic oxyhemoglobin. Accordingly, there should be an optimal pulmonary oxygen concentration for a given quantity of HP ¹²⁹Xe in the brain. In this study, the relationship between pulmonary oxygen concentration and HP ¹²⁹Xe signal in the brain was analyzed using a theoretical model and measured through in vivo experiments. The results from the theoretical model and experiments in rats are found to be in good agreement with each other. The optimal pulmonary oxygen concentration predicted by the theoretical model was 21%, and the in vivo experiments confirmed the presence of such an optimal ratio by reporting measurements between 25% and 35%. These findings are helpful for improving the ¹²⁹Xe signal in the brain and make the most of the limited spin polarization available for brain experiments. Copyright © 2016 John Wiley & Sons, Ltd.     

Preclinical hyperpolarized 129Xe MRI: ventilation and T2* mapping in mouse lungs at 7 T using multi‐echo flyback UTE

Fast apparent transverse relaxation (short T₂*) is a common obstacle when attempting to perform quantitative ¹H MRI of the lungs. While T₂* times are longer for pulmonary hyperpolarized (HP) gas functional imaging (in particular for gaseous ¹²⁹Xe), T₂* can still lead to quantitative inaccuracies for sequences requiring longer echo times (such as diffusion weighted images) or longer readout duration (such as spiral sequences). This is especially true in preclinical studies, where high magnetic fields lead to shorter relaxation times than are typically seen in human studies. However, the T₂* of HP ¹²⁹Xe in the most common animal model of human disease (mice) has not been reported. Herein, we present a multi‐echo radial flyback imaging sequence and use it to measure HP ¹²⁹Xe T₂* at 7 T under a variety of respiratory conditions. This sequence mitigates the impact of T₁ relaxation outside the animal by using multiple gradient‐refocused echoes to acquire images at a number of effective echo times for each RF excitation. After validating the sequence using a phantom containing water doped with superparamagnetic iron oxide nanoparticles, we measured the ¹²⁹Xe T₂* in vivo for 10 healthy C57Bl/6 J mice and found T₂* ~ 5 ms in the lung airspaces. Interestingly, T₂* was relatively constant over all experimental conditions, and varied significantly with sex, but not age, mass, or the O₂ content of the inhaled gas mixture. These results are discussed in the context of T₂* relaxation within porous media.     

Hyperpolarized 129Xe MRI using isobutene as a new quenching gas

The use of a quenching gas, isobutene, with a low vapor pressure was investigated to enhance the utility of hyperpolarized ¹²⁹Xe (HP Xe) MRI. Xenon mixed with isobutene was hyperpolarized using a home‐built apparatus for continuously producing HP Xe. The isobutene was then readily liquefied and separated almost totally by continuous condensation at about 173 K, because the vapor pressure of isobutene (0.247 kPa) is much lower than that of Xe (157 kPa). Finally, the neat Xe gas was continuously delivered to mice by spontaneous inhalation. The HP Xe MRI was enhanced twofold in polarization level and threefold in signal intensity when isobutene was adopted as the quenching gas instead of N₂. The usefulness of the HP Xe MRI was verified by application to pulmonary functional imaging of spontaneously breathing mice, where the parameters of fractional ventilation (r_a) and gas exchange (f_D) were evaluated, aiming at future extension to preclinical studies. This is the first application of isobutene as a quenching gas for HP Xe MRI.     

Reinvestigating hyperpolarized (129)Xe longitudinal relaxation time in the rat brain with noise considerations

The longitudinal relaxation time of hyperpolarized (HP) (129)Xe in the brain is a critical parameter for developing HP (129)Xe brain imaging and spectroscopy and optimizing the pulse sequences, especially in the case of cerebral blood flow measurements. Various studies have produced widely varying estimates of HP (129)Xe T(1) in the rat brain. To make improved measurements of HP (129)Xe T(1) in the rat brain and investigate how low signal-to-noise ratio (SNR) contributes to these discrepancies, we developed a multi-pulse protocol during the washout of (129)Xe from the brain. Afterwards, we applied an SNR threshold theory to both the multi-pulse protocol and an existing two-pulse protocol. The two protocols yielded mean +/- SD HP (129)Xe T(1) values in the rat brain of 15.3 +/- 1.2 and 16.2 +/- 0.9 s, suggesting that the low SNR might be a key reason for the wide range of T(1) values published in the literature, a problem that might be easily alleviated by taking SNR levels into account.     

Regional fractional ventilation mapping in spontaneously breathing mice using hyperpolarized 129Xe MRI

The feasibility of ventilation imaging with hyperpolarized (HP) ¹²⁹Xe MRI has been investigated for quantitative and regional assessment of ventilation in spontaneously breathing mice. The multiple breath ventilation imaging technique was modified to the protocol of spontaneous inhalation of HP ¹²⁹Xe delivered continuously from a ¹²⁹Xe polarizer. A series of ¹²⁹Xe ventilation images was obtained by varying the number of breaths before the ¹²⁹Xe lung imaging. The fractional ventilation, r, was successfully evaluated for spontaneously breathing mice. An attempt was made to detect ventilation dysfunction in the emphysematous mouse lung induced by intratracheal administration of porcine pancreatic elastase (PPE). As a result, the distribution of fractional ventilation could be visualized by the r map. Significant dysfunction of ventilation was quantitatively identified in the PPE‐treated group. The whole‐lung r value of 0.34 ± 0.01 for control mice (N = 4) was significantly reduced, to 0.25 ± 0.07, in PPE‐treated mice (N = 4) (p = 0.038). This study is the first application of multiple breath ventilation imaging to spontaneously breathing mice, and shows that this methodology is sensitive to differences in the pulmonary ventilation. This methodology is expected to improve simplicity as well as noninvasiveness when assessing regional ventilation in small rodents. Copyright © 2014 John Wiley & Sons, Ltd.     

Quantitative evaluation of pulmonary gas‐exchange function using hyperpolarized 129Xe CEST MRS and MRI

Hyperpolarized ¹²⁹Xe gas MR has been a powerful tool for evaluating pulmonary structure and function due to the extremely high enhancement in spin polarization, the good solubility in the pulmonary parenchyma, and the excellent chemical sensitivity to its surrounding environment. Generally, the quantitative structural and functional information of the lung are evaluated using hyperpolarized ¹²⁹Xe by employing the techniques of chemical shift saturation recovery (CSSR) and xenon polarization transfer contrast (XTC). Hyperpolarized ¹²⁹Xe chemical exchange saturation transfer (Hyper‐CEST) is another method for quantifying the exchange information of hyperpolarized ¹²⁹Xe by using the exchange of xenon signals according to its different chemical shifts, and it has been widely used in biosensor studies in vitro. However, the feasibility of using hyperpolarized ¹²⁹Xe CEST to quantify the pulmonary gas exchange function in vivo is still unclear. In this study, the technique of CEST was used to quantitatively evaluate the gas exchange in the lung globally and regionally via hyperpolarized ¹²⁹Xe MRS and MRI, respectively. A new parameter, the pulmonary apparent gas exchange time constant (T_app), was defined, and it increased from 0.63 s to 0.95 s in chronic obstructive pulmonary disease (COPD) rats (induced by cigarette smoke and lipopolysaccharide exposure) versus the controls with a significant difference (P = 0.001). Additionally, the spatial distribution maps of T_app in COPD rats' pulmonary parenchyma showed a regionally obvious increase compared with healthy rats. These results indicated that hyperpolarized ¹²⁹Xe CEST MR was an effective method for globally and regionally quantifying the pulmonary gas exchange function, which would be helpful in diagnosing lung diseases that are related to gas exchange, such as COPD.     

A protocol for quantifying cardiogenic oscillations in dynamic 129Xe gas exchange spectroscopy: The effects of idiopathic pulmonary fibrosis

The spectral parameters of hyperpolarized ¹²⁹Xe exchanging between airspaces, interstitial barrier, and red blood cells (RBCs) are sensitive to pulmonary pathophysiology. This study sought to evaluate whether the dynamics of ¹²⁹Xe spectroscopy provide additional insight, with particular focus on quantifying cardiogenic oscillations in the RBC resonance. ¹²⁹Xe spectra were dynamically acquired in eight healthy volunteers and nine subjects with idiopathic pulmonary fibrosis (IPF). ¹²⁹Xe FIDs were collected every 20 ms (T_E = 0.932 ms, 512 points, dwell time = 32 μs, flip angle ≈ 20°) during a 16 s breathing maneuver. The FIDs were pre‐processed using the spectral improvement by Fourier thresholding technique (SIFT) and fit in the time domain to determine the airspace, interstitial barrier, and RBC spectral parameters. The RBC and gas resonances were fit to a Lorentzian lineshape, while the barrier was fit to a Voigt lineshape to account for its greater structural heterogeneity. For each complex resonance the amplitude, chemical shift, linewidth(s), and phase were calculated. The time‐averaged spectra confirmed that the RBC to barrier amplitude ratio (RBC:barrier ratio) and RBC chemical shift are both reduced in IPF subjects. Their temporal dynamics showed that all three ¹²⁹Xe resonances are affected by the breathing maneuver. Most notably, several RBC spectral parameters exhibited prominent oscillations at the cardiac frequency, and their peak‐to‐peak variation differed between IPF subjects and healthy volunteers. In the IPF cohort, oscillations were more prominent in the RBC amplitude (16.8 ± 5.2 versus 9.7 ± 2.9%; P = 0.008), chemical shift (0.43 ± 0.33 versus 0.083 ± 0.05 ppm; P < 0.001), and phase (7.7 ± 5.6 versus 1.4 ± 0.8°; P < 0.001). Dynamic ¹²⁹Xe spectroscopy is a simple and sensitive tool that probes the temporal variability of gas exchange and may prove useful in discerning the underlying causes of its impairment.     

Continuous‐wave saturation considerations for efficient xenon depolarization

The combination of hyperpolarized Xe with chemical exchange saturation transfer (Hyper‐CEST) is a powerful NMR technique to detect highly dilute concentrations of Xe binding sites using RF saturation pulses. Crucially, that combination of saturation pulse strength and duration that generates the maximal Hyper‐CEST effect is a priori unknown. In contrast to CEST in proton MRI, where the system reaches a steady‐state for long saturation times, Hyper‐CEST has an optimal saturation time, i.e. saturating for shorter or longer reduces the Hyper‐CEST effect. Here, we derive expressions for this optimal saturation pulse length. We also found that a pulse strength, B₁, corresponding to five times the Xe exchange rate, k_BA (i.e. B₁ = 5 k_BA/γ with the gyromagnetic ratio of ¹²⁹Xe, γ), generates directly and without further optimization 96 % of the maximal Hyper‐CEST contrast while preserving spectral selectivity. As a measure that optimizes the amplitude and the width of the Hyper‐CEST response simultaneously, we found an optimal saturation pulse strength corresponding to times the Xe exchange rate, i.e. . When extremely low host concentration is detected, then the expression for the optimum saturation time simplifies as it approaches the longitudinal relaxation time of free Xe. Copyright © 2015 John Wiley & Sons, Ltd.     

Comparison of three reference methods for the measurement of intracellular pH using 31P MRS in healthy volunteers and patients with lymphoma

³¹P magnetic resonance spectroscopy (³¹P MRS) can measure intracellular pH (pH_i) using the chemical shift difference between pH‐dependent inorganic phosphate (P_i) and a pH‐independent reference peak. This study compared three different frequency reference peaks [phosphocreatine (PCr), α resonance of adenosine triphosphate (αATP) and water (using ¹H MRS)] in a cohort of 10 volunteers and eight patients with non‐Hodgkin's lymphoma (NHL). Well‐resolved chemical shift imaging (CSI) spectra were acquired on a 1.5T scanner for muscle, liver and tumour. The pH was calculated for all volunteers and patients using the available methods. The consistency of the resulting pH was evaluated. The direct P_i–PCr method was best for those spectra with a very well‐defined PCr, such as muscle (pH=7.05 ± 0.02). In liver, the P_i–αATP method gave more consistent results (pH=7.30 ± 0.06) than the calibrated water‐based method (pH=7.27 ± 0.11). In NHL nodes, the measured pH using the P_i–αATP method was 7.25 ± 0.12. Given that the measured range includes some biological variation in individual patients, treatment‐related changes of the order of 0.1 pH units should be detectable. © 2013 The Authors. NMR in Biomedicine published by John Wiley & Sons Ltd.     

MRI of stroke using hyperpolarized 129Xe

Because there is no background signal from xenon in biological tissue, and because inhaled xenon is delivered to the brain by blood flow, we would expect a perfusion deficit, such as is seen in stroke, to reduce the xenon concentration in the region of the deficit. Thermal polarization yields negligible xenon signal relative to hyperpolarized xenon; therefore, hyperpolarized xenon can be used as a tracer of cerebral blood flow. Using a rat permanent right middle cerebral artery occlusion model, we demonstrated that hyperpolarized ¹²⁹Xe MRI is able to detect, in vivo, the hypoperfused area of focal cerebral ischemia, that is the ischemic core area of stroke. To the best of our knowledge, this is the first time that hyperpolarized ¹²⁹Xe MRI has been used to explore normal and abnormal cerebral perfusion. Our study shows a novel application of hyperpolarized ¹²⁹Xe MRI for imaging stroke, and further demonstrates its capacity to serve as a complementary tool to proton MRI for the study of the pathophysiology during brain hypoperfusion. Copyright © 2010 John Wiley & Sons, Ltd.     

Cerebral blood flow response to acute hypoxic hypoxia

Hypoxic hypoxia (inspiratory hypoxia) stimulates an increase in cerebral blood flow (CBF) maintaining oxygen delivery to the brain. However, this response, particularly at the tissue level, is not well characterised. This study quantifies the CBF response to acute hypoxic hypoxia in healthy subjects. A 20‐min hypoxic (mean P_ETo ₂ = 52 mmHg) challenge was induced and controlled by dynamic end‐tidal forcing whilst CBF was measured using pulsed arterial spin labelling perfusion MRI. The rate constant, temporal delay and magnitude of the CBF response were characterised using an exponential model for whole‐brain and regional grey matter. Grey matter CBF increased from 76.1 mL/100 g/min (95% confidence interval (CI) of fitting: 75.5 mL/100 g/min, 76.7 mL/100 g/min) to 87.8 mL/100 g/min (95% CI: 86.7 mL/100 g/min, 89.6 mL/100 g/min) during hypoxia, and the temporal delay and rate constant for the response to hypoxia were 185 s (95% CI: 132 s, 230 s) and 0.0035 s^–1 (95% CI: 0.0019 s^–1, 0.0046 s^–1), respectively. Recovery from hypoxia was faster with a delay of 20 s (95% CI: –38 s, 38 s) and a rate constant of 0.0069 s^–1 (95% CI: 0.0020 s^–1, 0.0103 s^–1). R₂*, an index of blood oxygenation obtained simultaneously with the CBF measurement, increased from 30.33 s^–1 (CI: 30.31 s^–1, 30.34 s^–1) to 31.48 s^–1 (CI: 31.47 s^–1, 31.49 s^–1) with hypoxia. The delay and rate constant for changes in R₂* were 24 s (95% CI: 21 s, 26 s) and 0.0392 s^–1 (95% CI: 0.0333 s^–1, 0.045 s^–1 ), respectively, for the hypoxic response, and 12 s (95% CI: 10 s, 13 s) and 0.0921 s^–1 (95% CI: 0.0744 s^–1, 0.1098 s^–1/) during the return to normoxia, confirming rapid changes in blood oxygenation with the end‐tidal forcing system. CBF and R₂* reactivity to hypoxia differed between subjects, but only R₂* reactivity to hypoxia differed significantly between brain regions. © 2013 The Authors. NMR in Biomedicine published by John Wiley & Sons, Ltd.     

The effect of indomethacin on cerebral blood flow and oxygen consumption in the rat at normal and increased carbon dioxide tensions

The effect of the fatty acid cyclo-oxygenase inhibitor indomethacin on cerebral blood flow (CBF) and the metabolic rate for oxygen (CMRO₂) was studied in paralyzed and artificially ventilated rats. In normocapnic animals, the drug (10 mg·kg^-1i. v.) reduced CBF to 50% of control without a measurable effect on CMRO₂. During hypercapnia (Pa_CO2 70–80 mmHg) the increase in CBF was reduced by about 80% but CMRO₂ remained unchanged. Autoradiographic evaluation of local CBF in 20 brain structures indicated that the reduction in CBF was relatively uniform throughout the brain. Dose response curves showed that an effect on CBF was evident already at an indomethacin dose of 1 mg·kg^-1 and maximal effects were obtained with 3–5 mg·kg^-1. Following i. v. injection of the drug reduction in CBF was observed already after 10 s and the full response occurred after 1–2 min. It is concluded that metabolites of arachidonic acid, possibly mainly prostacyclin, are powerful modulators of normal cerebrovascular tone, and help to mediate the CBF response to increased CO₂ tensions. However, since indomethacin does not modify the circulatory response in other conditions with increased CBF these substances do not qualify as general coupling factors controlling CBF in physiological or pathological states.     

Glutamate receptor activation in cultured cerebellar granule cells increases cytosolic free Ca2+ by mobilization of cellular Ca2+ and activation of Ca2+ influx

Summary The Ca²⁺ sensitive fluorescent probe, fura-2 has been used to monitor cytosolic free calcium levels in mature primary cultures of cerebellar granule cells during exposure to L-glutamate and other excitatory amino acids: quisqualate (QA), kainate (KA) and N-methyl-D-aspartate (NMDA). Glutamate at micromolar concentrations produced a prompt and dose-related increase in the intracellular concentration of free Ca²⁺, ([Ca²⁺]_i), whereas QA, KA and NMDA had no effect. This increase was also seen in the absence of extracellular Ca²⁺, suggesting that L-glutamate promotes mobilization of Ca²⁺ from intracellular stores. In the presence of extracellular calcium, the elevation of [Ca²⁺]_i was, in part, mediated by an increase in the plasma membrane permeability to Ca²⁺. This Ca²⁺ influx was not affected by the Ca²⁺-channel antagonist 1-Verapamil. However, L-Verapamil did block the increase in [Ca²⁺]_i seen after depolarization of the cells with potassium. The Ca²⁺ response elicited by glutamate was partially blocked by the excitatory amino acid antagonist glutamate diethyl ester (GDEE). Furthermore, glutamate stimulated the formation of inositol mono-, bis-, tris and tetrakisphosphates (IP1, IP2, IP3, and IP4) suggesting a role for these compounds for the increase in [Ca²⁺]_i.     

31P‐MRS of healthy human brain: ATP synthesis,metabolite concentrations,pH, and T1 relaxation times

The conventional method for measuring brain ATP synthesis is ³¹P saturation transfer (ST), a technique typically dependent on prolonged pre‐saturation with γ‐ATP. In this study, ATP synthesis rate in resting human brain is evaluated using EBIT (exchange kinetics by band inversion transfer), a technique based on slow recovery of γ‐ATP magnetization in the absence of B₁ field following co‐inversion of PCr and ATP resonances with a short adiabatic pulse. The unidirectional rate constant for the P_i → γ‐ATP reaction is 0.21 ± 0.04 s^?1 and the ATP synthesis rate is 9.9 ± 2.1 mmol min^?1 kg^?1 in human brain (n = 12 subjects), consistent with the results by ST. Therefore, EBIT could be a useful alternative to ST in studying brain energy metabolism in normal physiology and under pathological conditions. In addition to ATP synthesis, all detectable ³¹P signals are analyzed to determine the brain concentration of phosphorus metabolites, including UDPG at around 10 ppm, a previously reported resonance in liver tissues and now confirmed in human brain. Inversion recovery measurements indicate that UDPG, like its diphosphate analogue NAD, has apparent T₁ shorter than that of monophosphates (P_i, PMEs, and PDEs) but longer than that of triphosphate ATP, highlighting the significance of the ³¹P–³¹P dipolar mechanism in T₁ relaxation of polyphosphates. Another interesting finding is the observation of approximately 40% shorter T₁ for intracellular P_i relative to extracellular P_i, attributed to the modulation by the intracellular phosphoryl exchange reaction P_i ? γ‐ATP. The sufficiently separated intra‐ and extracellular P_i signals also permit the distinction of pH between intra‐ and extracellular environments (pH 7.0 versus pH 7.4). In summary, quantitative ³¹P MRS in combination with ATP synthesis, pH, and T₁ relaxation measurements may offer a promising tool to detect biochemical alterations at early stages of brain dysfunctions and diseases. Copyright © 2015 John Wiley & Sons, Ltd.     

Hyperpolarized 13C magnetic resonance spectroscopy detects toxin‐induced neuroinflammation in mice

Lipopolysaccharide (LPS) is a commonly used agent for induction of neuroinflammation in preclinical studies. Upon injection, LPS causes activation of microglia and astrocytes, whose metabolism alters to favor glycolysis. Assessing in vivo neuroinflammation and its modulation following therapy remains challenging, and new noninvasive methods allowing for longitudinal monitoring would be highly valuable. Hyperpolarized (HP) ¹³C magnetic resonance spectroscopy (MRS) is a promising technique for assessing in vivo metabolism. In addition to applications in oncology, the most commonly used probe of [1–¹³C] pyruvate has shown potential in assessing neuroinflammation‐linked metabolism in mouse models of multiple sclerosis and traumatic brain injury. Here, we aimed to investigate LPS‐induced neuroinflammatory changes using HP [1–¹³C] pyruvate and HP ¹³C urea. 2D chemical shift imaging following simultaneous intravenous injection of HP [1–¹³C] pyruvate and HP ¹³C urea was performed at baseline (day 0) and at days 3 and 7 post‐intracranial injection of LPS (n = 6) or saline (n = 5). Immunofluorescence (IF) analyses were performed for Iba1 (resting and activated microglia/macrophages), GFAP (resting and reactive astrocytes) and CD68 (activated microglia/macrophages). A significant increase in HP [1–¹³C] lactate production was observed at days 3 and 7 following injection, in the injected (ipsilateral) side of the LPS‐treated mouse brain, but not in either the contralateral side or saline‐injected animals. HP ¹³C lactate/pyruvate ratio, without and with normalization to urea, was also significantly increased in the ipsilateral LPS‐injected brain at 7 days compared with baseline. IF analyses showed a significant increase in CD68 and GFAP staining at 3 days, followed by increased numbers of Iba1 and GFAP positive cells at 7 days post‐LPS injection. In conclusion, we can detect LPS‐induced changes in the mouse brain using HP ¹³C MRS, in alignment with increased numbers of microglia/macrophages and astrocytes. This study demonstrates that HP ¹³C spectroscopy has substantial potential for providing noninvasive information on neuroinflammation.     

The influence of obesity on cerebral blood flow in young adults using arterial spin labeling MRI

Obesity causes damage to several organs, including the brain. Recent studies have been focusing on understanding the mechanisms through which obesity affects brain structure and function using neuroimaging techniques. A functional biomarker, such as cerebral blood flow (CBF), is a powerful tool that can be used to explore neural dysfunction. However, there is currently limited information regarding the association between CBF and obesity. The study was conducted to investigate the potential effect of obesity on brain perfusion in a young cohort aged 20‐30 years. A total of 21 obese (body mass index (BMI) > 26 kg/m²) and 21 lean (BMI < 24 kg/m²) right‐handed volunteers were included in this study. CBF was acquired using the 2D single post‐labeling delay (PLD) arterial spin labeling (ASL) technique on a 3 T MRI scanner. A multiple regression analysis was performed to examine the difference in global and regional gray matter (GM) CBF between the groups. CBF value was assigned as the dependent variable, whereas age, sex, and group (obese or lean) were considered as the independent variables. Results showed that group‐related differences in CBF were homogeneous across brain regions, as obese subjects had significantly lower global GM CBF than lean subjects (P < 0.05). In the voxelwise analysis, obese individuals had significantly lower CBF in the left pulvinar of the thalamus and visual association areas, including Brodmann area (BA) 7, BA18, and BA19, than lean subjects. Although the signal‐to‐noise ratio was slightly compromised for 2D sequences and subject‐specific arterial transit time was not estimated due to a single PLD sequence, this study demonstrated alterations in CBF in obese subjects, particularly in regions of the pulvinar of the thalamus and its synchronously related areas such as visual association areas. These results suggest that ASL provides a potential platform for further obesity‐related research.     

MRI of cerebral blood flow under hyperbaric conditions in rats

Hyperbaric oxygen (HBO) therapy has a number of clinical applications. However, the effects of acute HBO on basal cerebral blood flow (CBF) and neurovascular coupling are not well understood. This study explored the use of arterial spin labeling MRI to evaluate changes in baseline and forepaw stimulus‐evoked CBF responses in rats (n = 8) during normobaric air (NB), normobaric oxygen (NBO) (100% O ₂ ), 3 atm absolute (ATA) hyperbaric air (HB) and 3 ATA HBO conditions. T ₁ was also measured, and the effects of changes in T ₁ caused by increasing oxygen on the CBF calculation were investigated. The major findings were as follows: (i) increased inhaled oxygen concentrations led to a reduced respiration rate; (ii) increased dissolved paramagnetic oxygen had significant effects on blood and tissue T ₁ , which affected the CBF calculation using the arterial spin labeling method; (iii) the differences in blood T ₁ had a larger effect than the differences in tissue T ₁ on CBF calculation; (iv) if oxygen‐induced changes in blood and tissue T ₁ were not taken into account, CBF was underestimated by 33% at 3 ATA HBO, 10% at NBO and <5% at HB; (v) with correction, CBF values under HBO, HB and NBO were similar (p > 0.05) and all were higher than CBF under NB by ~40% (p < 0.05), indicating that hypercapnia from the reduced respiration rate masks oxygen‐induced vasoconstriction, although blood gas was not measured; and (vi) substantial stimulus‐evoked CBF increases were detected under HBO, similar to NB, supporting the notion that activation‐induced CBF regulation in the brain does not operate through an oxygen‐sensing mechanism. CBF MRI provides valuable insights into the effects of oxygen on basal CBF and neurovascular coupling under hyperbaric conditions. Copyright © 2016 John Wiley & Sons, Ltd.     

Real‐time measurement of hyperpolarized lactate production and efflux as a biomarker of tumor aggressiveness in an MR compatible 3D cell culture bioreactor

We have developed a 3D cell/tissue culture bioreactor compatible with hyperpolarized (HP) ¹³C MR and interrogated HP [1‐¹³C]lactate production and efflux in human renal cell carcinoma (RCC) cells. This platform is capable of resolving intracellular and extracellular HP lactate pools, allowing the kinetic measurement of lactate production and efflux in the context of cancer aggressiveness and response to therapy. HP ¹³C MR studies were performed on three immortalized human renal cell lines: HK2, a normal renal proximal tubule cell line from which a majority of RCCs arise, UMRC6, a cell line derived from a localized RCC, and UOK262, an aggressive and metastatic RCC. The intra‐ (Lac_in) and extracellular (Lac_ex) HP lactate signals were robustly resolved in dynamic ¹³C spectra of the cell lines due to a very small but reproducible chemical shift difference (0.031 ± 0.0005 ppm). Following HP [1‐¹³C]pyruvate delivery, the ratio of HP Lac_in/Lac_ex was significantly lower for UOK262 cells compared with both UMRC6 and HK2 cells due to a significant (p < 0.05) increase in the Lac_ex pool size. Lac_in/Lac_ex correlated with the MCT4 mRNA expression of the cell lines, and inhibition of MCT4 transport using DIDS resulted in a significant reduction in the HP Lac_ex pool size. The extension of these studies to living patient‐derived RCC tissue slices using HP [1,2‐¹³C₂]pyruvate demonstrated a similarly split lactate doublet with a high Lac_ex pool fraction; in contrast, only a single NMR resonance is noted for HP [5‐¹³C]glutamate, consistent with intracellular localization. These studies support the importance of lactate efflux as a biomarker of cancer aggressiveness and metastatic potential, and the utility of the MR compatible 3D cell/tissue culture bioreactor to study not only cellular metabolism but also transport. Additionally, this platform offers a sophisticated way to follow therapeutic interventions and screen novel therapies that target lactate export. Copyright © 2015 John Wiley & Sons, Ltd.     

Pacing-Induced Non-Uniform Ca2+ Dynamics in Rat Atria Revealed by Rapid-Scanning Confocal Microscopy

Intracellular Ca²⁺ ([Ca²⁺]_i) dynamics in isolated myocytes differ between the atria and ventricles due to the distinct t-tubular distributions. Although cellular aspects of ventricular [Ca²⁺]_i dynamics in the heart have been extensively studied, little is known about those of atrial myocytes in situ. Here we visualized precise [Ca²⁺]_i dynamics of atrial myocytes in Langendorff-perfused rat hearts by rapid-scanning confocal microscopy. Of 16 fluo-4-loaded hearts imaged during pacing up to 4-Hz, five hearts showed spatially uniform Ca²⁺ transients on systole among individual cells, whereas no discernible [Ca²⁺]_i elevation developed during diastole. In contrast, the remaining hearts showed non-uniform [Ca²⁺]_i dynamics within and among the cells especially under high-frequency (4 Hz) excitation, where subcellular cluster-like [Ca²⁺]_i rises or wave-like [Ca²⁺]_i propagation occurred on excitation. Such [Ca²⁺]_i inhomogeneity was more pronounced at high-frequency pacing, showing beat-to-beat Ca²⁺ transient alternans. Despite such non-uniform dynamics, cessation of burst pacing of the atria was not followed by emergence of spontaneous Ca²⁺ waves, indicating minor Ca²⁺-releasing potentials of the sarcoplasmic reticulum (SR). In summary, rat atria display a propensity to show non-uniform [Ca²⁺]_i dynamics on systole due to impaired Ca²⁺-release from the SR and paucity of t-tubules. Our results provide an important basis for understanding atrial pathophysiology.     

A Method for Determining Blood Flow and Oxygen Consumption in the Rat Brain

Cerebral blood flow (CBF) and cerebral metabolic rate for oxygen (CMRo₂) were measured in rats under nitrous oxide anaesthesia, using a ¹³³Xenon modification of the Kety and Schmidt inert gas technique with sampling of cerebral venous blood from the retroglenoid vein. Extracerebral contamination of the venous blood sampled was studied by comparing the rates at which the activity of ¹³³Xenon decreased in blood and tissues. Contamination was avoided by gentle compression of the contralateral retroglenoid vein during sampling. CBF and CMRo₂ of the rat brain were 80±2 and 7.6 ± 0.2 ml·(100 g)^-1, min^-1, respectively. These values are about 25% lower than those previously obtained for cerebral cortical tissue under similar conditions. Induced hypercapnia (Paco₂ about 70 mm Hg) or hypocapnia (Paco² 15–20 mm Hg) gave rise to expected changes in CBF but did not alter CMRo² The CMRo² of the rat brain is at least twice that of the human brain. This species difference, which is similar to that previously reported for the oxygen uptake of cerebral tissue in vitro, probably reflects on inverse relationship between brain weight and neuronal packing density.