Abstract
Over the past decade there has been an enormous progress in our understanding of fluid and solute transport in the central nervous system (CNS). This is due to a number of factors, including important developments in whole brain imaging technology and computational fluid dynamics analysis employed for the elucidation of glymphatic transport function in the live animal and human brain. In this paper, we review the technical aspects of dynamic contrast enhanced magnetic resonance imaging (DCE-MRI) in combination with administration of Gd-based tracers into the cerebrospinal fluid (CSF) for tracking glymphatic solute and fluid transport in the CNS as well as lymphatic drainage. Used in conjunction with advanced computational processing methods including optimal mass transport analysis, one gains new insights into the biophysical forces governing solute transport in the CNS which leads to intriguing new research directions. Considering drainage pathways, we review the novel T1 mapping technique for quantifying glymphatic transport and cervical lymph node drainage concurrently in the same subject. We provide an overview of knowledge gleaned from DCE-MRI studies of glymphatic transport and meningeal lymphatic drainage. Finally, we introduce positron emission tomography (PET) and CSF administration of radiotracers as an alternative method to explore other pharmacokinetic aspects of CSF transport into brain parenchyma as well as efflux pathways.
Background
This review focuses on technical aspects and new knowledge of fluid and solute transport via the glymphatic system and connected drainage pathways gained over the last decade using magnetic resonance imaging (MRI) and positron emission tomography (PET). However, a brief historical overview on cerebrospinal fluid (CSF) transport research is appropriate given the considerable knowledge gained from these now classical studies. Roy Mott (Mott, 1910) and Weed (Weed, 1922) were among the earliest anatomists to conceptualize and describe CSF flow via peri-vascular conduits in the central nervous system (CNS). In Weed’s book on CSF, the peri-vascular fluid channels were referred to as ‘lymphatic’ in character (Weed, 1922). Weed (Weed, 1922) and Halliburton (Halliburton, 1917) further documented that the perivascular fluid channels acted as communication routes between subarachnoid fluid and interstitial fluid (ISF) of neuropil. Importantly, Weed highlighted that ‘in comparison to blood flow, velocities of the CSF are slow and more difficult to measure” (Weed, 1922). Several decades later, Weller described the Virchow-Robin spaces around the large arteries as they enter the normal human brain and their complex leptomeningeal sheaths and connections to the subarachnoid space (Weller et al., 1992). He further emphasized that the perivascular space for CSF passage along the penetrating arteries became virtual conduits comprising only the basement membrane at the level of the capillary bed (Weller, et al., 1992). In 1985, Rennels and coworkers pioneered new dynamic information on rapid brain-wide perivascular solute movement (Rennels et al., 1985). They infused horseradish peroxidase into CSF via the lateral ventricle or cisterna magna of the cat brain and noted rapid (~4min) distribution of the tracer surrounding all penetrating arterioles across brain structures (Rennels, et al., 1985). Notably, they also showed that arterial pulsations were required for the rapid perivascular solute flow (Rennels, et al., 1985). Several reviews on CSF flow and CNS homeostasis are available and the interested reader is referred to these for more detail (Abbott et al., 2018, Hladky and Barrand, 2014, Johnston, 2003, Louveau et al., 2015, Louveau et al., 2017, Raper et al., 2016). Fast-forwarding to 2012, Iliff and Nedergaard introduced the glymphatic system as a brain-wide perivascular transit passageway for CSF facilitating waste clearance from the brain in a manner dependent on glial cells and aquaporin 4 (AQP4) water channels (Iliff et al., 2012, Mestre et al., 2018).
Waste and solute drainage via the glymphatic system have been studied extensively in the live rodent brain (Ding et al., 2018, Gaberel et al., 2014, Huber et al., 2018, Iliff et al., 2014, Lee et al., 2015, Morris et al., 2016, Yang et al., 2013), non-human primate brain (Goulay et al., 2018, Ohno et al., 2019), and human brain (Eide and Ringstad, 2015, Eide and Ringstad, 2018, Ringstad et al., 2017), and is conceptualized as a dynamic 3-step process: (1) bulk-flow driven influx of CSF from the peri-arterial compartment into interstitial fluid (ISF); (2) CSF-ISF mixing in the neuropil driving extracellular waste solutes towards peri-venous conduits; and (3) exit of waste solutes from peri-venous conduits into lymphatic vessels with subsequent systemic absorption and metabolic breakdown (Iliff, et al., 2012). The working hypothesis of solute and fluid transport through the glymphatic system is still under investigation, in particular, the issue of direction and biophysical forces underlying solute flow in neuropil. The current controversies pertaining to glymphatic transport and solute movement in CSF and neuropil can be researched in several reviews and the interested reader is referred to these for more information (Abbott, et al., 2018, Benveniste et al., 2019, Brinker et al., 2014, Mestre et al., 2020, Wardlaw et al., 2020). In regards to characterization and further understanding of the lymphatic exit pathways this has been accomplished by the creation of lymphatic endothelial cell-specific fluorescent reporter mice and immunofluorescent staining for lymphatics such as LYVE-1, PROX-1 and VEGFR-3 (Truman et al., 2013). Thus, an intricate but rather sparse network of bona fide lymphatic vessels in the dura mater of the brain was uncovered (Aspelund et al., 2015, Louveau et al., 2015) and spinal cord (Antila et al., 2017, Jacob et al., 2019) and shown to drain specific anatomical districts of lymph nodes (Antila, et al., 2017, Da Mesquita et al., 2018, Jacob, et al., 2019, Louveau et al., 2018, Louveau, et al., 2015).
Glymphatic system transport captured in vivo by dynamic contrast enhanced MRI
The need to capture brain-wide glymphatic solute transport in real time was essential to further define transport kinetics and for exploring the physiological drivers of the system. Although, post-mortem approaches provided proof of peri-arterial influx of small molecular weight (MW) tracers from CSF into ISF, the unavoidable tissue processing including formalin-fixation affected uptake patterns and therefore data interpretation (Mestre et al., 2018). For example, from the first glymphatic system study it was shown that small molecular weight (MW) fluorescently tagged tracers like Texas-red distributed very rapidly (~30min after CSF administration) from CSF into ISF across the whole brain (Iliff, et al., 2012). It has now been repeatedly shown by in vivo imaging (vide infra) that extracellular tracer distribution from CSF into all regions of the brain is rather slow because glymphatic transport kinetics across brain regions is heterogeneous (Iliff et al., 2013, Lee, et al., 2015).
MRI which is an inherently three-dimensional (3D) and non-invasive technique was an obvious first choice for exploring glymphatic system transport dynamics in the live rodent brain (Iliff, et al., 2013). Spatial resolution and endogenous tissue contrast of MRI images acquired at high magnetic field was excellent for visualizing brain anatomy and larger vascular structures necessary for interpreting glymphatic system fluid and solute fluxes across compartments. Specifically, dynamic contrast enhanced MRI (DCE-MRI) using a 3D T1-weighted pulse sequence, in combination with CSF administration of paramagnetic contrast molecules was used for visualizing glymphatic system transport in the whole rat brain (Iliff, et al., 2013). Given the reported slower velocity ranges of CSF flow when compared to blood flow (Haughton et al., 2003), the temporal resolution of DCE-MRI was also suitable to capture macro- and mesoscale biophysical kinetic patterns of glymphatic solute transport (Lee, et al., 2015, Mortensen et al., 2019). In the first study of glymphatic transport in rat brain by DCE-MRI, the rat with the indwelling CSF catheter in the cisterna manga (Fig. 1A) was placed supine with the small RF surface coils positioned underneath the head (Fig. 1B). In two different series of rats, gadopentetate dimeglumine (Gd-DTPA, MW 938 Da) or the larger MW polymeric Gd-chelate GadoSpin (200,000 Da) was administered into the CSF via a small catheter implanted into the cisterna magna of rats anesthetized with a long-acting barbiturate (Iliff, et al., 2013). The small and large MW paramagnetic contrast molecules were used to validate the previously reported presence of bulk flow along the peri-arterial CSF influx routes (Iliff, et al., 2012, Rennels, et al., 1985). If peri-arterial transport is driven by bulk flow, solute speed would be independent of the contrast molecule’s MW. To compare glymphatic transport between Gd-DTPA and GadoSpin their respective T1 relaxation effects had to be matched and 0.17 mM GadoSpin and 21 mM Gd-DTPA solutions were determined to fulfill these requirements (Iliff, et al., 2013). We note that a large volume of the paramagnetic contrast solute was delivered intrathecally (80 μl at a rate of 1.6 μl/min) with the goal of ‘saturating’ and achieving sufficient contrast enhancement in all brain regions. The DCE-MRI data was acquired using a dynamic 3D T1-weighted FLASH sequence acquired over ~4.2 hrs. To visualize glymphatic transport of the tracer, the DCE-MRI data were converted into parametric maps in which the signal intensity of each voxel represented ‘percentage signal change from the baseline’ also referred to as the ‘enhancement ratio’ (Iliff, et al., 2013). Fig. 1 shows whole brain glymphatic uptake patterns of Gd-DTPA (Figs. 1C–E) and GadoSpin (Figs. 1F–H) ~90 min following contrast administration. Glymphatic transport is presented as a 3D volume rendered color-coded map overlaid on the corresponding anatomical template of the rat brain. It is evident that there is more tissue uptake of Gd-DTPA in comparison to GadoSpin. Parenchymal uptake of Gd-DTPA is extensive especially in the cerebellum and along ventral surface (brainstem, pons, hypothalamus), ventral hippocampus, and olfactory bulb (Figs. 1C–E). GadoSpin with a MW of 200,000 Da has restricted access from the perivascular space via the astrocytic end-feet gaps (~20–30nM) to ISF, and it therefore accumulates in the subarachnoid CSF and the perivascular space of the larger pial surface arteries as well as along dural sinuses (Figs. 1F–H). Several investigators have reproduced this characteristic spatial distribution pattern of glymphatic transport with different paramagnetic agents in a wide variety of animal species including human brain using DCE-MRI (Table 1). In the following sections we will highlight key technical features that have been refined over time. Further, the parametric quantitative output of solute and fluid transport as well as new knowledge of glymphatic system function revealed by DCE-MRI is presented in Table 2.
Table 1:
Species | Anesthesia | Contrast agent/molecular weight (MW) | Contrast concentration (mM) | Volume and infusion rate | Magnetic field & sequence | Spatial resolution (mm3) | Year [Reference] |
---|---|---|---|---|---|---|---|
Rat | Nembutal | Gd-DTPA, MW 938 Da and GadoSpin P (MW 200 kDa; | 21 mM Gd-DTPA; 0.17 mM GadoSpin | 80 μl 1.6μl/min |
9.4T 3D T1-weighted FLASH |
0.117 × 0.234 × 0.250 = 0.007 mm3 | 2013 (Iliff, et al., 2013) |
Mouse | Isoflurane/NO2 | Gadoterate meglumine (DOTAREM) | 500mM DOTA-Gd (DOTAREM®, | 1μ 1μ/min |
7.0T 3D T1-weighted FLASH |
0.078 × 0.078 × 0.150 = 0.001 mm3 | 2014 (Gaberel, et al., 2014) |
Rat | Ketamine/Xylazine | Gd-DTPA, MW 938 Da | 12.5 mM Gd-DTPA | 20 μl 1 μl/min |
9.4T 3D T1-weighted FLASH; T1 mapping |
0.12 × 0.12 × 0.13 mm = 0.002 mm3 | 2015 (Lee, et al., 2015) |
Human | N/A | Gadobutrol | 1000mM | Bolus injection | 1.5T 3D T1 weighted sequence |
Not reported | 2015 (Eide and Ringstad, 2015) |
Rat | Isoflurane | Gd-DTPA, MW 938 Da | 21 mM Gd-DTPA | 80 μl 1.6μl/min |
7.0T 3D T1-weighted FLASH |
0.125 × 0.1 25 × 0.125 mm = 0.002 mm3 | 2017 (Jiang et al., 2016) |
Rat | Dexmedeto midine/Isoflurane | Gd-DTPA, MW 938 Da | 12.5 mM Gd-DTPA | 20 μl 1.7μl/min |
9.4T 3D T1-weighted FLASH |
0.12 × 0.12 × 0.13 mm = 0.002 mm3 | 2017 (Benveniste, et al., 2017) |
Human | N/A, Awake | Gadobutrol | 1000mM gadobutrol | 0.5 ml Bolus injection | 3T sagittal 3D T1-weighted scans |
1 × 1 × 1 mm = 1 mm3 | 2017 (Ringstad, et al., 2017) |
Mouse | Isoflurane; Ketamine/Xylazine | Gd-DTPA, MW 938 Da | 500mM DOTA-Gd (DOTAREM®) | 1-3 μL 1μ/min |
7.0T 3D T1-weighted FLASH |
0.078 × 0.078 × 0.150 = 0.001 mm3 | 2018 (Gakuba et al., 2018) |
Rat | Dexmedeto midine + low dose Isoflurane | Gadoterate meglumine (DOTAREM) | 13.5 mM | 20 μL 1.5 μl/min |
9.4T 3D T1-weighted FLASH |
0.24 × 0.24 × 0.26 mm =0.015 mm3 | 2018 (Lee, et al., 2018) |
Human | N/A, Awake | Gadobutrol | 1000mM | 0.5 ml Bolus injection | 3T sagittal 3D T1-weighted scan |
1 × 1 × 0.5 mm = 0.5 mm3 | 2018 (Ringstad et al., 2018) |
Mouse | Ketamine/Xylazine | Gadoteridol (68mM, osmotically adjusted) | 68 mM | 10 μL 0.5 μl/min |
11.75 T 3D FLASH |
0.1 × 0.1 × 0.1 mm = 0.001 mm3 | 2018 (Mestre, et al., 2018) |
Nonhuman primate | Isoflurane | Gadoteridol | 2mM | 1ml/min | 1.5T T1-weighted |
unclear | 2018 (Ohno, et al., 2019) |
Rat | Isoflurane/NO2 | Gd-DTPA | 21.7 mM | 1.17 μL/min 1.67 μL/min 2.92 μL/min |
7.0T 3D T1-weighted FLASH |
0.125 × 0.1 67 × 0.167 mm = 0.003 mm3 | 2018 (Ding, et al., 2018) |
Rat | Isoflurane | Gd-DTPA | 21 mM | 80 μl at 1.6 μl/min & 4 μl at 0.4 μl/min, | 9.4 T | ? | 2019 (Hadjihambi et al., 2019) |
Rat | Dexmedeto midine + low dose Isoflurane | Gadoterate meglumine (DOTAREM) | 13.5 mM | 20 μL 1.5 μL/min |
9.4T VFA-SPGR sequence |
0.24 × 0.24 × 0.26 mm (0.015 mm3) | 2019 (Mortensen, et al., 2019) |
Rat | Dexmedeto midine + low dose Isoflurane | Gadoterate meglumine (DOTAREM) | 13.5mM and 100mM | 20 μl 1.5 μL/mi n |
9.4T VFA-SPGR sequence |
0.30 × 0.30 × 0.30 mm 0.15 × 0.15 × 0.15 mm | 2020 (Koundal, et al., 2020) |
Table 2:
Species | Route of Contrast | Glymphatic Parameters Measured | Physiological State or Disease? | Knowledge Gained | References |
---|---|---|---|---|---|
Rat | Intracisternal | - Time-activity curve - Cluster analysis |
Physiological | - Visualized the paraarterial CSF pathways and areas of CSF-ISF exchange - Tracer size affects its distribution in the brain |
2013 (Iliff, et al., 2013) |
Mouse | Intracisternal | Visualization of contrast distribution throughout the brain | Various vascular pathologies | Glymphatic impairment was evident following subarachnoid hemorrhage and ischemic stroke, but not after common carotid artery occlusion and intracerebral hemorrhage | 2014 (Gaberel, et al., 2014) |
Rat | Intralumbar | Flow kinetics | Physiological | Utilized optimal mass transfer (OMT) method to create a glymphatic flow model | 2015 (Ratner et al., 2015) |
Rat | Intracisternal | - Time-signal curve - Flow kinetics |
Physiological | Glymphatic transport was affected by body position and was most efficient in the right lateral decubitus position | 2015 (Lee, et al., 2015) |
Human | Intralumbar | T1 signal intensities of ROIs | Intracranial hypotension caused by CSF leakage | Contrast-enhanced MRI may be a viable technique for glymphatic studies in humans | 2015 (Eide and Ringstad, 2015) |
Human | Intravenous | T2 signal intensities of ROIs | Physiological | Intravenous contrast can enter the perivascular spaces via the CSF | 2017 (Naganawa et al., 2017) |
Rat | Intracisternal | Flow kinetics | Physiological | Improved upon previous work (Ratner, et al., 2015) on an optimal mass transfer (OMT) method to model glymphatic flow | 2017 (Ratner, et al., 2017) |
Rat | Intracisternal | - Time-evolution curve - Residual intensity - Clearance rate - Cluster analysis |
Type 2 diabetes mellitus | - Glymphatic transport was impaired in rats with type 2 diabetes mellitus - Increased retention of contrast in the hippocampus and hypothalamus of rats with type 2 diabetes mellitus |
2017 (Jiang et al., 2017) |
Nonhuman Primate | Intracisternal | - Visualization of contrast distribution throughout the brain - T1 signal intensities of ROIs |
Subarachnoid hemorrhage | Subarachnoid hemorrhage significantly impaired circulation of CSF through the parenchyma | 2017 (Goulay et al., 2017) |
Human | Intralumbar | - Time-signal curve - Clearance rate - T1 signal intensities of ROIs |
Idiopathic normal pressure hydrocephalus | - Distribution of contrast throughout the brain was slower in humans when compared to rats - Glymphatic transport was decreased in patients with idiopathic normal pressure hydrocephalus, possibly due to restricted arterial pulsation |
2017 (Ringstad, et al., 2017) |
Rat | Intracisternal | - Time-signal curve - Clearance rate |
Physiological | Glymphatic transport was increased in rats anesthetized with lowdose isoflurane supplemented with dexmedetomidine when compared to rats anesthetized with only isoflurane | 2017 (Benveniste, et al., 2017) |
Mouse | Intracisternal | - Visualization of contrast distribution throughout the brain - T1 signal intensities of ROIs |
Physiological | First study to show that glymphatic transport was decreased with anesthesia when compared to the awake state, in contrast to most other studies. | 2018 (Gakuba, et al., 2018) |
Rat | Intracisternal | - Visualization of contrast distribution throughout the brain - T1 signal intensities of ROIs - Time-activity curve |
Physiological | Introduction of a B1+ correction factor for more accurate T1/contrast measurements | 2018 (Lee, et al., 2018) |
Human | Intralumbar | T1 signal intensities of ROIs | Various CSF disorders | - Contrast drains from the CSF into the cervical lymph nodes - Drainage from nasal lymphatics and perineural pathways may be less pronounced in humans compared to rats |
2018 (Eide et al., 2018) |
Human | Intralumbar | - Visualization of contrast distribution throughout the brain - Time-signal curve - Clearance rate - T1 signal intensities of ROIs |
Idiopathic normal pressure hydrocephalus | Clearance, but not uptake, of contrast was decreased in patients with idiopathic normal pressure hydrocephalus | 2018 (Ringstad, et al., 2018) |
Rat | Intravenous | - Time-signal curve - T1 signal intensities of ROIs |
Physiological | - Signal intensity in the fourth ventricle increased immediately after intravenous contrast injection, suggesting the CSF as a potential intermediary pathway for contrast in the blood to reach the brain - Time-of-day of contrast injections may affect brain contrast concentrations |
2018 (Taoka et al., 2018) |
Rat Mouse | Intracisternal | - Visualization of contrast distribution throughout the brain - T1 signal intensities of ROIs |
Physiological | Both flow and efflux of CSF increases as newborn rats and mice mature into adults | 2018 (Di Palma et al., 2018) |
Mouse | Intracisternal | - Visualization of contrast distribution throughout the brain - T1 signal intensities of ROIs |
AQP4 knockout | A meta-analysis of five studies (using both microscopy and DCEMRI) strongly reinforced the theory that AQP4 facilitates the influx of CSF into the parenchyma | 2018 (Mestre, et al., 2018) |
Rat | Intracisternal | - Time-evolution curve - T1 signal intensities of ROIs |
Physiological | - Described the effect of various contrast infusion rates on distribution and clearance Higher infusion rates show quicker distribution of contrast, but with a higher risk of disturbing CSF flow 2018 |
(Ding, et al., 2018) |
Rat | Intracisternal | - Visualization of contrast distribution throughout the brain - Time-signal curve |
Physiological | Introduced a mathematical model of the glymphatic system using local, rather than global, input functions | 2019 (Davoodi-Bojd, et al., 2019) |
Nonhuman Primate | - Intracisternal - Intralumbar - Intraventricular |
- Visualization of contrast distribution throughout the brain - Clearance rate |
Physiological | Distribution and clearance of tracer varies between different contrast delivery methods, with acute cisterna magna injection achieving the quickest and most extensive coverage of the brain | 2019 (Ohno, et al., 2019) |
Rat | Intracisternal | - Visualization of contrast distribution throughout the brain - Time-signal curve - T1 signal intensities of ROIs |
Chronic liver disease with minimal hepatic encephalopathy | Both influx and clearance of contrast in the frontal brain was decreased in rats with chronic liver disease, possibly due to decreased expression of aquaporin-4 in this region | 2019 (Hadjihambi, et al., 2019) |
Mouse | Intracisternal | - Visualization of contrast distribution throughout the brain and spinal cord - T1 signal intensities of ROIs |
Experimental autoimmune encephalomyelitis (multiple sclerosis model) | Parenchymal CSF circulation in the spinal cord, but not the brain, was decreased in mice with a model of multiple sclerosis, possibly due to leukocyte infiltration | 2019 (Fournier et al., 2019) |
Phantom | N/A | T2 signal intensities of ROIs | N/A | Increasing repetition time (TR) helped increase the signal intensity of low concentration contrast, suggesting that higher TR may be utilized to detect low contrast concentrations in certain locations and after extended durations | 2019 (Kato et al., 2019) |
Human | Intravenous | T2 signal intensities of ROIs | Blood-brain barrier damage | Contrast in the blood may enter the CSF by way of the choroid plexus, aqueous humour, and/or trigeminal nerve | 2019 (Deike-Hofmann et al., 2019) |
Human | Intralumbar | - Visualization of contrast distribution throughout the brain - Concentrationtime curve |
Physiological | Quantified contrast concentration in the human brain over a period of 3 days | 2019 (Watts, et al., 2019) |
Human | Intralumbar | T1 signal intensities of ROIs | Physiological | Contrast injected into the spinal subarachnoid space accessed the visual pathways, suggesting the existence of an ocular glymphatic system | 2019 (Jacobsen et al., 2019) |
Rat | Intracisternal | - Visualization of contrast distribution throughout the brain -Timeconcentration curve -Flow kinetics |
Spontaneous hypertension | - Developed a new compartmental model to analyze contrast influx and efflux - Glymphatic influx and efflux was reduced in adult spontaneously hypertensive rats |
2019 (Mortensen, et al., 2019) |
Human | Intralumbar | Time for contrast to reach level of the foramen magnum (spinal transit time) | Various CSF disorders | - Intrathecal contrast injection is safe in humans without allergies to contrast - Contrast in the spinal cord reached the intracranial CSF in 99 out of 100 patients |
2019 (Edeklev et al., 2019) |
Human | Intravenous | Visualization of T1 signal intensities | Ultrasound-induced blood-brain barrier damage | Introduced a method of transient local blood-brain barrier opening to facilitate contrast penetration from the blood into the brain, allowing for local noninvasive visualization of the glymphatic system | 2019 (Meng et al., 2019) |
Human | Intralumbar | T1 and T2 signal intensities of ROIs | Various neurological diseases | - Simultaneously imaged the brain, putative meningeal lymph vessels, and deep cervical lymph nodes in humans, allowing for visualization of the glymphatic clearance pathways - Showed that clearance through these pathways may be impaired with aging |
2020 (Zhou et al., 2020) |
Human | Intravenous | Visualization of contrast distribution along vessels/sinuses | Physiological | The space under the pial sheath of cortical vessels may be connected with meningeal lymphatics | 2020 (Naganawa et al., 2020) |
Rat | Intraventricular | T1 signal intensities of ROIs | Physiological | - Intraventricular injection of contrast may be plausible in glymphatic imaging - The distribution of contrast was more widespread during the dark phase of a light-dark cycle |
2020 (Cai et al., 2020) |
Rat | Yes | - Visualization of contrast distribution throughout the brain - Flow kinetics |
Spontaneous hypertension | - Applied a novel method to reveal the contributions of advective and diffusive forces to glymphatic transport - Solute flow speed was reduced in spontaneously hypertensive rats |
2020 (Koundal, et al., 2020) |
Human | Intralumbar | - Time-signal curve - T1 signal intensities of ROIs |
Physiological | Established a physiological baseline of CSF contrast kinetics in various cortical and subcortical areas of the human brain | 2020 (Dyke et al., 2020) |
Rat | Intracisternal | - Time-evolution curve - T1 signal intensities of ROIs |
Ischemic stroke | - During the acute phase, clearance of contrast was slower in the hemisphere ipsilateral to ischemia - During the subacute phase, contrast’s time-to-peak was longer and its retention was increased ipsilateral to ischemia |
2020 (Lin et al., 2020) |
Mouse | Intracisternal | - Visualization of contrast distribution throughout the brain - T1 signal intensities of ROIs |
Physiological | - Introduced a new method of glymphatic transport quantification and analysis - Contrast drains from the brain into the deep cervical and submandibular lymph nodes |
2020 (Xue, et al., 2020) |
Rat | Intracisternal | - Time-signal curves - T1 signal intensities of ROIs |
AQP4 inhibition | - Inhibition of AQP4 led to decreased influx of contrast into the parenchyma | 2020 (Takano and Yamada, 2020) |
Rat | Intracisternal | - Visualization of contrast distribution throughout the brain - Time-signal curves - Flow kinetics |
Mild traumatic brain injury | Both glymphatic influx and clearance was persistently impaired during the chronic time course following mild traumatic brain injury | 2020 (Li et al., 2020) |
CSF infusion rate, total Gd contrast mass and volume for glymphatic transport by MRI
When performing glymphatic studies using DCE-MRI and Gd-based contrast administration into CSF it is important that the intracranial pressure (ICP) remains within normal limits during the experiment. A higher than normal ICP will affect cerebral blood flow and if severely elevated will compromise tissue perfusion, induce ischemia leading to cytotoxic edema and decreases in the ISF volume fraction which will adversely impact glymphatic transport (Mestre et al., 2020). Conversely, a lower than normal ICP can emerge if CSF is leaking during the cisterna magna cannulation (or deliberately via cisternotomy (Plog et al., 2015)) or if the experiment is conducted in the setting of an open, unsealed craniotomy with dura removed. Regardless, any alteration of ICP from normal levels will change intracranial hydraulic pressure gradients and impact glymphatic transport dynamics. Table 1 shows that the total Gd-based contrast volume used in glymphatic studies are generally adjusted to the physical size of the CSF compartment of the species to avoid excessive ICP changes. For example, the CSF compartment volume determined by anatomical MRI in normal rat and mouse is ~250μl (Lee et al., 2020) and ~40μl (Ma et al., 2008), respectively. Further, the CSF production rate in adult mice is ~0.35μl/min (Pardridge, 2016) and ~1.5μl/min in young adult rats (Karimy et al., 2015). Considering these numbers, Gd-contrast volumes in the range of ~20–30 μl infused at rates of 0.5–3μl/min (Ding, et al., 2018) used in glymphatic rat studies are physiologically reasonable and associated with only minor transient increases in ICP (Koundal et al., 2020). Similarly, for mice, Gd-contrast volumes in the range of 1–10μl using infusion rates of ~1–2μl/min are regarded to be safe and associated with minor, transient increases in ICP (Xue et al., 2020). However, these recommendations are based on experiments conducted in spontaneously breathing rodents anesthetized with a wide variety of hypnotic and anesthetic agents, which affect ICP differently and thus CSF infusion conditions. Several studies listed in Table 1 have recorded only subtle elevations of ICP during the CSF infusion and it is therefore inferred that unphysiological ICP conditions did not impact glymphatic transport dynamics.
Differences across DCE-MRI studies in regard to Gd-contrast concentration and total ‘mass’ delivered into CSF (Table 1) is a tradeoff between achieving sufficient Gd-contrast uptake in the whole brain for detection by T1-weighted MR contrast (T1 shortening) while not ‘overshooting’ the local Gd tissue concentration, which would induce unwanted susceptibility T2* and signal loss (Lee et al., 2018). Another issue to consider in DCE-MRI studies is the baricity of the Gd-contrast mixture administered into CSF. Baricity is the ratio of the density of a local anesthetic solution to the density of CSF. Density is defined as the mass per unit volume of solution (g/mL) and the density of CSF is 1.0004–1.0006 g/L. If the Gd-contrast mixture has the same density as CSF it is ‘isobaric’, and those with higher and lower density than CSF are hyperbaric and hypobaric, respectively. A commonly used Gd-based molecule for glymphatic studies is the commercially available gadoterate meglumine delivered as an aqueous 500mM solution (Dotarem®, Gerbet LLC, France). In the manufacturer’s formulation, the density of Dotarem (a.k.a. Gd-DOTA) is given as 1.1753 g/ml and the osmolarity as 1350 mOsm/kg water (Agency). Thus, administering Gd-DOTA in a concentrated formulation which is hyperbaric as well as hyperosmotic compared to CSF (osmolarity of normal CSF ~285–290 mOsm/kg) might influence the distribution pattern and transport kinetics assessed via the glymphatic system. Currently there is a gap in knowledge as to how baricity and osmotic pressure of the contrast/tracer solutions affect glymphatic transport data and more studies are needed to clarify these issues. Fig. 2 shows an example of a glymphatic DCE-MRI study with CSF Gd-DOTA administered in a 1:5 dilution in combination with a small RF surface coil positioned over the left hemisphere of an anesthetized rat (Koundal, et al., 2020). These technical implementations were done specifically to increase perivascular Gd-contrast enhancement along the middle cerebral artery and enabled documentation of perivascular solute and fluid transport impairment in a rat model of chronic hypertension (Koundal, et al., 2020).
Glymphatic transport and body posture
For glymphatic transport experiments it is important to track physiological parameters carefully including stability of the anesthetic state. Most glymphatic transport studies are carried out in anesthetized, spontaneously breathing rodents positioned either supine or prone with the head fixed in a stereotaxic frame or head holder (so-called sphinx position). The body position used for glymphatic transport experiments in rodents is important because each head/body position (e.g. supine, prone, or lateral recumbent) are associated with diverse changes in several physiological parameters including ICP, central venous pressure and heart rate. We previously investigated the effect of body position on glymphatic transport in anesthetized rodents (Lee, et al., 2015). Our study showed that the prone sphinx position with the head above the heart decreased glymphatic transport and clearance of soluble Aβ in comparison from the neuropil in comparison to supine and lateral recumbent body positions (Lee, et al., 2015). Thus, in the sleeping or anesthetized state where the glymphatic system is vigorously engaged in solute and fluid transport (when compared to wakefulness) (Xie et al., 2013) the most beneficial sleeping positions from the point of view of waste clearance would be supine and/or lateral recumbent body positions. Interestingly, studies have shown that the right lateral sleeping position is the most favored by adult humans (De Koninck et al., 1992). According to reports from veterinarians and wild-life scientists, rodents sleep ‘naturally’ in groups with other rats to bond and share warmth and this can include a wide range of body postures. However, in experimental settings or single caged housing, rodents’ sleeping positions are lateral, ‘curled up’ with the head tucked in towards the legs. Ideally, glymphatic studies should be carried out in the most physiological correct conditions, and lateral recumbent body posture with the head gently bent might be more ‘natural’ when compared to supine body position. However, in many experimental setting including MRI imaging with physiological monitoring and indwelling CSF catheters this may be difficult to mimic the ‘natural’ sleeping position of the given species studied; and this should be considered with interpreting glymphatic transport data.
T1 mapping technique for quantifying glymphatic and lymphatic transport
In glymphatic studies, the enhancement ratio (ER) defined as % signal change from the baseline is a semi-quantitative technique that is simple to calculate and easy to interpret because in normal brain tissue, ER values are proportional to the Gd concentration (Benveniste et al., 2017, Harrison et al., 2020, Lee, et al., 2018, Lee, et al., 2015). However, ER data obtained in neurodegenerative disease states should be interpreted with care because pathophysiological conditions (e.g. stroke, hemorrhage or brain injury) alters the tissue T1 when compared to normal healthy tissue (Barbier et al., 2005). When the pre-contrast T1 of the pathological tissue is significantly different from normal values, the relationship between the ER and Gd concentration also changes and this can lead to inaccurate conclusions. For example, if the T1 is different between normal and pathological tissue the ER may erroneously reflect this difference but in fact the Gd concentration (and glymphatic solute transport) might remain unchanged. To circumvent this problem, and to derive accurate glymphatic solute transport measures it is necessary to calculate the actual Gd concentration (mM) instead of using the ER. To this end, we developed a 3D T1 mapping technique using 3D variable flip angle spoiled gradient echo sequence (VFA-SPGR) and processing algorithms for converting ER to Gd concentrations (Lee, et al., 2018, Mortensen, et al., 2019). The VFA-SPGR protocol comprises acquisition of SPGR images at multiple flip angles and the protocol can be implemented easily since it does not require specialized hardware or pulse sequences. However, it is well known that T1 derived from VFA-SPGR data can be inaccurate in the presence of substantial RF transmit coil inhomogeneity (B1+) resulting in spatially heterogeneous flip angle, which deviate from the nominal flip angle. Therefore B1+ correction is essential for calculating accurate VFA-SPGR T1 maps (Lee, et al., 2018). Using T1 mapping wtih Gd concentration calculations we previously estimated that only ~20% of Gd contrast was transported into the brain from the CSF (cisterna magna) inferring that the bulk of tracer mass does not enter the brain-wide glymphatic system but migrate to spine and or drains directly to the lymphatics (Lee, et al., 2018, Lee, et al., 2015, Xue, et al., 2020).
The T1 mapping technique is also advantageous for quantifying glymphatic transport as well as drainage of the Gd contrast solute to the cervical lymph nodes (superficial as well as deep cervical lymph nodes) in vivo (Xue, et al., 2020). Fig. 3 shows the T1 mapping approach for quantifying glymphatic transport and cervical lymphatic drainage in a mouse anesthetized with ketamine/xylazine. With this particular technique, the Gd-DOTA is administered on the bench, and the CSF catheter is removed after the injection prior to MRI scanning which, makes the set up less technically challenging and more time efficient (Xue, et al., 2020). The first T1 map is acquired approximately 1 hr after the administration of contrast and represents a single ‘snapshot’ of glymphatic transport and lymphatic drainage at this time point (Xue, et al., 2020). The field-of-view of the T1 maps includes the head and neck of the mouse so glymphatic Gd-DOTA and drainage of Gd-DOTA to the cervical lymph nodes can be quantified in the same mouse (Fig. 3). The superficial (submandibular) cervical lymph nodes are located rostral to the submandibular gland (Figs. 3A, B) while the deep cervical lymph nodes are located lateral and posterior to the trachea and common carotid arteries (Figs. 3C, D). The cervical lymph nodes appear ‘dark’ after Gd-DOTA drainage because of T1 shortening which lowers the T1 by ~30–205% when compared to normal T1 tissue values (Figs. 3E, F). The glymphatic transport and drainage of Gd-DOTA to the cervical lymph nodes are quantified by measuring the number voxels of T1 values at a specific range (e.g. 1–1800 ms) and this volume can then be compared to control mice (normal T1 values ~2000ms) (Xue, et al., 2020). A similar approach can be used in human DCE-MRI studies though parenchymal uptake and clearance of contrast requires days rather than hours and data must be collected over multiple visits (Ringstad, et al., 2017, Watts et al., 2019).
Quantification of glymphatic transport from DCE-MRI data
In order to interpret DCE-MRI glymphatic studies and how this technology have contributed to knowledge on the system’s function in normal and diseased brain it is important to briefly discuss how solute and fluid transport is quantified. In the following we will discuss glymphatic system transport quantification by K-means cluster analysis, kinetic tissue compartment modeling and optimal mass transport processing.
K-means cluster analysis:
Glymphatic influx of the Gd-based contrast solute into brain was originally quantified across regions and in whole brain using ‘time-signal’ curves (time-to-peak and ‘area under curve time-integrals) as well as k-means cluster analysis (Iliff, et al., 2013). Fig. 4 shows an example of k-means 3-cluster analysis using a DCE-MRI glymphatic study with CSF Gd-DOTA administration from a normal 3M old Sprague Dawley rat. The 3 tissue compartments defined by k-means cluster analysis are shown as binary volume rendered color-coded masks overlaid on the corresponding anatomical brain (Figs. 4B–D). While the red cluster is located in the CSF compartment proper and includes the basal cisterns (Fig. 4B) the blue cluster is ‘parenchymal’ (Fig 4D). The green cluster represents an mixed cluster comprising subarachnoid CSF, CSF in the peri-vascular compartments of large arteries as well as adjacent tissue (Fig. 4C). The corresponding time signal curves (TSC) from the three clusters are shown in Fig. 4E. The red cluster’s TSC represents the smallest tissue compartment (2487 voxels) and is characterized by high peak magnitude (~300% signal increase) and rapid decay (Fig. 4E). The parenchymal TSC represents the largest tissue volume (10015 voxels) and is characterized by low signal magnitude and slow decay (Fig. 4D). More details and further development of the cluster analysis approach for glymphatic system transport analysis can be found in Davoodi-Bojd et al. (Davoodi-Bojd et al., 2019).
Tissue compartment kinetic modeling:
We previously extracted TSCs from CSF and tissue compartments from DCE-MRI studies focused on characterizing the effect of different body postures on glymphatic system transport in rodents (Lee, et al., 2015). We used a Logan plot to calculate the tissue distribution volume V(t) of the Gd-DTPA tracer over the predefined time (~3hrs) and implemented a 2-tissue compartment model to derive information on tracer tissue ‘retention’ and ‘loss’ (Lee, et al., 2015). The 2-compartment model allowed us to incorporate the slower and heterogeneous movement of Gd-contrast more accurately in the brain tissue compartment in comparison to CSF and peri-arterial conduits. More recently, we used the CSF and tissue TSCs to model and quantify glymphatic transport kinetics using a 1-tissue compartment model and TSC representing Gd-concentrations derived from the T1 mapping approach (Mortensen, et al., 2019). Fig. 4 shows the processing steps involved in the 1-tissue compartment analysis from CSF and brain tissue compartments. The first step involves segmenting the corresponding anatomical template for the DCE-MRI glymphatic study into a CSF and parenchymal compartment using voxel based morphometric analysis (Koundal et al., 2019, Lee, et al., 2020). The TSC from the CSF and tissue compartments are used as input into the 1-compartment model to derive the influx and efflux rate constants as well as the total tissue distribution volume (Fig. 4).
Regularized Optimal Mass Transport (rOMT):
The 1-tissue compartment kinetic model fits whole brain data derived from DCE-MRI and CSF Gd-contrast delivery well and rate constants for quantifying influx and efflux. However, the kinetic tissue models but often fails at the local tissue level due to glymphatic transport heterogeneity as well as in disease states when glymphatic solute transport is compromised. To obtain information on dynamic glymphatic transport at the voxel-level in the live brain we have instead employed methods from optimal mass transport (OMT) (Ratner et al., 2017, Villani, 2009) including a regularized version to study the glymphatic systems (Elkin et al., 2018). The regularized OMT (rOMT) problem is concerned with the minimization of the kinetic energy functional wherein the advection/diffusion equation is the only a priori assumption required; (for more detail see (Koundal, et al., 2020)). The rOMT analysis returns the interpolated density images and velocity fields. We further implemented the Lagrangian formulation for visualizing glymphatic transport flows over a specific time interval (Koundal, et al., 2020). From the Lagrangian pathlines several biophysical measures can be derived including the total flow volume (size of the pathline network), and the glymphatic transport speed across tissue compartments. Fig. 5 shows examples of rOMT glymphatic analysis of DCE-MRI Gd-DOTA data from a rat anesthetized with dexmedetomidine supplemented with low dose isoflurane. The dynamic information of solute transport within the brain and efflux pathways derived from rOMT analysis is unique. For example, the color-coded local speed map shows that solute speed trajectories are fast in the CSF compartment and slow down in parenchyma (Fig. 5B). The velocity flux vector analysis captures the direction and strength (vector magnitude) of solute movement over the pre-defined time window. Along the circle of Willis on the ventral surface of the brain, solute transport from the perivascular space into parenchyma can be appreciated (Figs. 5C, D). For more details about rOMT data interpretation see Koundal et al., (Koundal, et al., 2020).
Glymphatic system evaluated by 2-deoxy-2-[18F]fluoroglucose PET-CT
Here we also want to introduce a novel approach to capture glymphatic transport and drainage using PET-CT in combination with administration of 2-deoxy-2-[18F]fluoroglucose (18FDG) into CSF. Positron emission tomography (PET) technology allows to measure with high sensitivity the concentration of positron labelled radiotracers as a function of time in living tissues (Alluri et al., 2020, Fowler et al., 2003, Fowler et al., 2004, Volkow et al., 2003). In the brain the use of PET in combination with a diverse set of radiotracers has been used to measure the regional brain concentration of receptors, enzymes and transporters as well as the transport and pharmacokinetics of molecules such as acetate or of drugs such as cocaine (Ashok et al., 2017, Fowler et al., 1999, Volkow et al., 2013, Volkow et al., 2017). PET has also been used to measure physiological processes such as glucose metabolism, which is done using 18FDG a surrogate of glucose that is trapped intracellularly when it is phosphorylated by hexokinase as part of the metabolic cycle (Fowler and Ido, 2002, Fowler, et al., 2004). Typically, PET studies are performed by injecting the radiotracer intravenously and measuring its concentration in the brain (or other tissues). In our PET studies to study the glymphatic system in the rat we injected 18FDG into the CSF via the cisterna magna in order to measure the pharmacokinetics of FDG from CSF into the brain tissue. To compare the CSF data with the conventional intravenous (i.v.) administration we also included rats who received 18FDG intravenously. For the glymphatic experiments, we anesthetized 4 female rats with barbiturate (see supplemental methods) and acquired a CT scan covering the head and thorax followed by a dynamic PET scans obtained at 5-min intervals for a total of ~1.5 hours. For the i.v. experiments we anesthetized 4 female rats with barbiturates and after the CT scan the 18FDG dynamic PET scans were obtained at 5-min intervals for a total of 1 hr using the same field-of-view as for the CSF experiments. Fig. 6 shows 3D volume rendered color-coded 18FDG brain images overlaid on the corresponding anatomical CT images obtained at different times after 18FDG administration. Figs. 6A–C show the 18FDG uptake from CSF and at the initial scan times 18FDG is distributed mainly in the basal cistern (cisterna magna) and spinal column space and after 60 minutes 18FDG can be observed along the ventral surface of the CSF, in the brain tissue, nasal conchae as well as in the heart. At 90 min there is increased uptake in brain and nasal conchae. The corresponding time activity curves (TAC) are shown in Fig. 6G and demonstrate that 18FDG activity peaks at ~25min from the time of CSF administration and then decays over time. TACs from the nasal conchae (representing glymphatic ‘efflux’) show a slow and steady increase after 20min of CSF circulation (Fig. 6G). For comparison, we also show corresponding the dynamic 18FDG images after intravenous administration obtain in the other series of rats (Figs. 6D–F). The 18FDG TAC from brain and nasal conchae after i.v. administration of the radiotracer shows rapid increase and reaches a plateau after ~35min where the 18FDG is trapped intracellularly as has been shown previously (Shimoji et al., 2004).
Although this is a preliminary study, the time course of 18FDG uptake is clearly different for the CSF vs. i.v. administration and suggests rich possibilities for analysis, from more complex kinetic models to simple ratio measures that might reflect clearance rates. For example, at late times (>70 min after CSF administration) the brain and nasal conchae levels change relatively linearly with time (brain decreasing and conchae increasing), suggesting that the ratio of conchae to brain is also a stable linear function of time whose slope may be quite sensitive to clearance rate from the brain. Although the spatial resolution of PET is generally inferior to MRI, these studies suggest that it is sufficient for the study of the glymphatic system in the rat brain on at least global and regional scales. An important advantage is that fully quantified PET images directly reflect mass concentrations of the tracer with minimal assumptions with no inherent dependence on disease state of the tissue. Moreover, to avoid potentially confounding effects of anesthesia, PET studies can be carried out in the conscious state using multiple approaches (Kyme et al., 2018, Miranda et al., 2019, Schulz et al., 2011). As such, PET could develop into a standalone approach to the study of glymphatic function, and/or be used to validate the MRI approaches using dual-labeled probes and the new generation of simultaneous PET/MRI scanners. In addition, alternate PET radio-lαβeled tracers should be considered apart from 18FDG which is a metabolically active molecule which is trapped by brain cells and therefore would not easily provide information on efflux or ‘clearance’ from glymphatic to the lymphatic drainage routs. Another metabolically active tracer would be 15O-water which when injected into the cisterna magna could track water movement from CSF spaces into brain parenchyma and theoretically would have the ability to quantify the movement of water - driven by osmotic active substances - in neuropil and via the glymphatic system. However, a limitation is the very short half-life (2 min) of 15O-water which would limit its application for studying glymphatic-lymphatic transport in the live CNS. Potential alternate tracer candidates for PET based studies of glymphatic and lymphatic transport would ideally be metabolically inert molecules. In DCE-MRI studies Gd-tagged small MW metabolically inert molecules are typically used which are transported in CSF and interstitial fluid of the CNS and which do not normally cross the blood brain barrier. Such radioligands would include 18F-labeled albumin which has gained some interest for lymphatic imaging (Wang et al., 2015) and which should track glymphatic transport in a pattern similar to that observed in DCE-MRI studies and theoretically also efflux to the lymphatic system. Finally, for studying amyloid beta (Aβ) clearance radiotracers that bind to soluble Aβ would be needed which currently are not available. Clearly more studies are needed to explore the full potential of PET for the study of glymphatic system function.
Supplementary Material
Highlights:
Dynamic contrast enhanced MRI and CSF delivery of Gd-based contrast agents is a robust imaging platform for quantifying brain-wide glymphatic transport
Glymphatic transport and CSF flow dynamics is dependent on body posture
T1 mapping by MRI can quantify glymphatic transport and drainage to cervical lymph nodes concurrently in the same subject
Glymphatic transport kinetics are heterogenous across brain regions
Dynamic solute and fluid transport in the CNS by optimal mass transport analysis requires incorporation of advective as well as diffusion terms
Glymphatic transport can be measured by positron emission tomography with CSF administration of radioactive ligands
Footnotes
Conflicts of interest: None
Financial disclosures: NIH R01AG048769, RF1 AG053991, R01AG057705 and Leducq Foundation (16/CVD/05)
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