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MRI pulse sequence

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This table does not include uncommon and experimental sequences.

Group Sequence Abbr. Physics Main clinical distinctions Example
Spin echo T1 weighted T1 Measuring spin–lattice relaxation by using a short repetition time (TR) and echo time (TE).

Standard foundation and comparison for other sequences

T2 weighted T2 Measuring spin–spin relaxation by using long TR and TE times
  • Higher signal for more water content[1]
  • Low signal for fat in standard Spine Echo (SE),[1] though not with Fast Spin Echo/Turbo Spin Echo (FSE/TSE). FSE/TSE is the standard of care in modern medicine because it is faster. With FSE/TSE, fat has high signal due to disruption of hyperfine J-coupling between adjacent fat protons.[3]
  • Low signal for paramagnetic substances[2]

Standard foundation and comparison for other sequences

Proton density weighted PD Long TR (to reduce T1) and short TE (to minimize T2).[4] Joint disease and injury.[5]
Gradient echo (GRE) Steady-state free precession SSFP Maintenance of a steady, residual transverse magnetisation over successive cycles.[7] Creation of cardiac MRI videos (pictured).[7]
Effective T2
or "T2-star"
T2* Spoiled gradient recalled echo (GRE) with a long echo time and small flip angle[8] Low signal from hemosiderin deposits (pictured) and hemorrhages.[8]
Susceptibility-weighted SWI Spoiled gradient recalled echo (GRE), fully flow compensated, long echo time, combines phase image with magnitude image[9] Detecting small amounts of hemorrhage (diffuse axonal injury pictured) or calcium.[9]
Inversion recovery Short tau inversion recovery STIR Fat suppression by setting an inversion time where the signal of fat is zero.[10] High signal in edema, such as in more severe stress fracture.[11] Shin splints pictured:
Fluid-attenuated inversion recovery FLAIR Fluid suppression by setting an inversion time that nulls fluids High signal in lacunar infarction, multiple sclerosis (MS) plaques, subarachnoid haemorrhage and meningitis (pictured).[12]
Double inversion recovery DIR Simultaneous suppression of cerebrospinal fluid and white matter by two inversion times.[13] High signal of multiple sclerosis plaques (pictured).[13]
Diffusion weighted (DWI) Conventional DWI Measure of Brownian motion of water molecules.[14] High signal within minutes of cerebral infarction (pictured).[15]
Apparent diffusion coefficient ADC Reduced T2 weighting by taking multiple conventional DWI images with different DWI weighting, and the change corresponds to diffusion.[16] Low signal minutes after cerebral infarction (pictured).[17]
Diffusion tensor DTI Mainly tractography (pictured) by an overall greater Brownian motion of water molecules in the directions of nerve fibers.[18]
Perfusion weighted (PWI) Dynamic susceptibility contrast DSC Measures changes over time in susceptibility-induced signal loss due to gadolinium contrast injection.[20]
  • Provides measurements of blood flow
  • In cerebral infarction, the infarcted core and the penumbra have decreased perfusion and delayed contrast arrival (pictured).[21]
Arterial spin labelling ASL Magnetic labeling of arterial blood below the imaging slab, which subsequently enters the region of interest.[22] It does not need gadolinium contrast.[23]
Dynamic contrast enhanced DCE Measures changes over time in the shortening of the spin–lattice relaxation (T1) induced by a gadolinium contrast bolus.[24] Faster Gd contrast uptake along with other features is suggestive of malignancy (pictured).[25]
Functional MRI (fMRI) Blood-oxygen-level dependent imaging BOLD Changes in oxygen saturation-dependent magnetism of hemoglobin reflects tissue activity.[26] Localizing brain activity from performing an assigned task (e.g. talking, moving fingers) before surgery, also used in research of cognition.[27]
Magnetic resonance angiography (MRA) and venography Time-of-flight TOF Blood entering the imaged area is not yet magnetically saturated, giving it a much higher signal when using short echo time and flow compensation. Detection of aneurysm, stenosis, or dissection[28]
Phase-contrast magnetic resonance imaging PC-MRA Two gradients with equal magnitude, but opposite direction, are used to encode a phase shift, which is proportional to the velocity of spins.[29] Detection of aneurysm, stenosis, or dissection (pictured).[28]
(VIPR)

Diffusion MRI

DTI image

Diffusion MRI measures the diffusion of water molecules in biological tissues.[30] Clinically, diffusion MRI is useful for the diagnoses of conditions (e.g., stroke) or neurological disorders (e.g., multiple sclerosis), and helps better understand the connectivity of white matter axons in the central nervous system.[31] In an isotropic medium (inside a glass of water for example), water molecules naturally move randomly according to turbulence and Brownian motion. In biological tissues however, where the Reynolds number is low enough for laminar flow, the diffusion may be anisotropic. For example, a molecule inside the axon of a neuron has a low probability of crossing the myelin membrane. Therefore, the molecule moves principally along the axis of the neural fiber. If it is known that molecules in a particular voxel diffuse principally in one direction, the assumption can be made that the majority of the fibers in this area are parallel to that direction.

The recent development of diffusion tensor imaging (DTI)[32] enables diffusion to be measured in multiple directions, and the fractional anisotropy in each direction to be calculated for each voxel. This enables researchers to make brain maps of fiber directions to examine the connectivity of different regions in the brain (using tractography) or to examine areas of neural degeneration and demyelination in diseases like multiple sclerosis.

Another application of diffusion MRI is diffusion-weighted imaging (DWI). Following an ischemic stroke, DWI is highly sensitive to the changes occurring in the lesion.[33] It is speculated that increases in restriction (barriers) to water diffusion, as a result of cytotoxic edema (cellular swelling), is responsible for the increase in signal on a DWI scan. The DWI enhancement appears within 5–10 minutes of the onset of stroke symptoms (as compared to computed tomography, which often does not detect changes of acute infarct for up to 4–6 hours) and remains for up to two weeks. Coupled with imaging of cerebral perfusion, researchers can highlight regions of "perfusion/diffusion mismatch" that may indicate regions capable of salvage by reperfusion therapy.

Like many other specialized applications, this technique is usually coupled with a fast image acquisition sequence, such as echo planar imaging sequence.

Steady-state free precession imaging

Steady-state free precession imaging (SSFP MRI) is an MRI technique which uses steady states of magnetizations. In general, SSFP MRI sequences are based on a (low flip angle) gradient-echo MRI sequence with a short repetition time which in its generic form has been described as the FLASH MRI technique. While spoiled gradient-echo sequences refer to a steady state of the longitudinal magnetization only, SSFP gradient-echo sequences include transverse coherences (magnetizations) from overlapping multi-order spin echoes and stimulated echoes. This is usually accomplished by refocusing the phase-encoding gradient in each repetition interval in order to keep the phase integral (or gradient moment) constant. Fully balanced SSFP MRI sequences achieve a phase of zero by refocusing all imaging gradients.

New methods and variants of existing methods are often published when they are able to produce better results in specific fields. Examples of these recent improvements are T*
2
-weighted
turbo spin-echo (T2 TSE MRI), double inversion recovery MRI (DIR-MRI) or phase-sensitive inversion recovery MRI (PSIR-MRI), all of them able to improve imaging of brain lesions.[34][35] Another example is MP-RAGE (magnetization-prepared rapid acquisition with gradient echo),[36] which improves images of multiple sclerosis cortical lesions.[37]

Magnetization transfer MRI

Magnetization transfer (MT) is a technique to enhance image contrast in certain applications of MRI.

Bound protons are associated with proteins and as they have a very short T2 decay they do not normally contribute to image contrast. However, because these protons have a broad resonance peak they can be excited by a radiofrequency pulse that has no effect on free protons. Their excitation increases image contrast by transfer of saturated spins from the bound pool into the free pool, thereby reducing the signal of free water. This homonuclear magnetization transfer provides an indirect measurement of macromolecular content in tissue. Implementation of homonuclear magnetization transfer involves choosing suitable frequency offsets and pulse shapes to saturate the bound spins sufficiently strongly, within the safety limits of specific absorption rate for MRI.[38]

The most common use of this technique is for suppression of background signal in time of flight MR angiography.[39] There are also applications in neuroimaging particularly in the characterization of white matter lesions in multiple sclerosis.[40]

T1rho MRI

T1ρ (T1rho): Molecules have a kinetic energy that is a function of the temperature and is expressed as translational and rotational motions, and by collisions between molecules. The moving dipoles disturb the magnetic field but are often extremely rapid so that the average effect over a long time-scale may be zero. However, depending on the time-scale, the interactions between the dipoles do not always average away. At the slowest extreme the interaction time is effectively infinite and occurs where there are large, stationary field disturbances (e.g., a metallic implant). In this case the loss of coherence is described as a "static dephasing". T2* is a measure of the loss of coherence in an ensemble of spins that includes all interactions (including static dephasing). T2 is a measure of the loss of coherence that excludes static dephasing, using an RF pulse to reverse the slowest types of dipolar interaction. There is in fact a continuum of interaction time-scales in a given biological sample, and the properties of the refocusing RF pulse can be tuned to refocus more than just static dephasing. In general, the rate of decay of an ensemble of spins is a function of the interaction times and also the power of the RF pulse. This type of decay, occurring under the influence of RF, is known as T1ρ. It is similar to T2 decay but with some slower dipolar interactions refocused, as well as static interactions, hence T1ρ≥T2.[41]

Proton density weighted

Proton density (PD) weighted images are created by having a long repetition time (TR) and a short echo time (TE).[42] On images of the brain, this sequence has a more pronounced distinction between gray matter (bright) and white matter (darker gray), but with little contrast between brain and CSF.[42]

Fluid attenuated inversion recovery (FLAIR)

Fluid attenuated inversion recovery (FLAIR)[43] is an inversion-recovery pulse sequence used to nullify the signal from fluids. For example, it can be used in brain imaging to suppress cerebrospinal fluid (CSF) so as to bring out periventricular hyperintense lesions, such as multiple sclerosis (MS) plaques. By carefully choosing the inversion time TI (the time between the inversion and excitation pulses), the signal from any particular tissue can be suppressed.

Susceptibility weighted imaging (SWI)

Susceptibility weighted imaging (SWI) is a new type of contrast in MRI different from spin density, T1, or T2 imaging. This method exploits the susceptibility differences between tissues and uses a fully velocity compensated, three dimensional, RF spoiled, high-resolution, 3D gradient echo scan. This special data acquisition and image processing produces an enhanced contrast magnitude image very sensitive to venous blood, hemorrhage and iron storage. It is used to enhance the detection and diagnosis of tumors, vascular and neurovascular diseases (stroke and hemorrhage), multiple sclerosis,[44] Alzheimer's, and also detects traumatic brain injuries that may not be diagnosed using other methods.[45]

Fast spin

Fast spin echo (FSE), also called turbo spin echo (TSE) is a sequence that results in fast scan times. In this sequence, several 180 refocusing radio-frequency pulses are delivered during each echo time (TR) interval, and the phase-encoding gradient is briefly switched on between echoes.[46]

Fat suppression

Fat suppression is useful for example to distinguish active inflammation in the intestines from fat deposition such as can be caused by long-standing (but possibly inactive) inflammatory bowel disease, but also obesity, chemotherapy and celiac disease.[47] Techniques to suppress fat on MRI mainly include:[48]

  • Identifying fat by the chemical shift of its atoms, causing different time-dependent phase shifts compared to water.
  • Frequency-selective saturation of the spektral peak of fat by a "fat sat" pulse before imaging.
  • Short tau inversion recovery (STIR), a T1-dependent method
  • Spectral presaturation with inversion recovery (SPIR)

Neuromelanin imaging

This method exploits the paramagnetic properties of neuromelanin and can be used to visualize the substantia nigra and the locus coeruleus. It is used to detect the atrophy of these nuclei in Parkinson's disease and other parkinsonisms, and also detects signal intensity changes in major depressive disorder and schizophrenia.[49]

References

  1. ^ a b c d "Magnetic Resonance Imaging". University of Wisconsin. Archived from the original on 2017-05-10. Retrieved 2016-03-14.
  2. ^ a b c d Johnson KA. "Basic proton MR imaging. Tissue Signal Characteristics". Harvard Medical School. Archived from the original on 2016-03-05. Retrieved 2016-03-14.
  3. ^ Henkelman, RM; Hardy, PA; Bishop, JE; Poon, CS; Plewes, DB (September 1992). "Why fat is bright in RARE and fast spin-echo imaging". Journal of magnetic resonance imaging : JMRI. 2 (5): 533–40. doi:10.1002/jmri.1880020511. PMID 1392246.
  4. ^ Graham D, Cloke P, Vosper M (2011-05-31). Principles and Applications of Radiological Physics E-Book (6 ed.). Elsevier Health Sciences. p. 292. ISBN 978-0-7020-4614-8.}
  5. ^ du Plessis V, Jones J. "MRI sequences (overview)". Radiopaedia. Retrieved 2017-01-13.
  6. ^ Lefevre N, Naouri JF, Herman S, Gerometta A, Klouche S, Bohu Y (2016). "A Current Review of the Meniscus Imaging: Proposition of a Useful Tool for Its Radiologic Analysis". Radiology Research and Practice. 2016: 8329296. doi:10.1155/2016/8329296. PMC 4766355. PMID 27057352.
  7. ^ a b Luijkx T, Weerakkody Y. "Steady-state free precession MRI". Radiopaedia. Retrieved 2017-10-13.
  8. ^ a b Chavhan GB, Babyn PS, Thomas B, Shroff MM, Haacke EM (2009). "Principles, techniques, and applications of T2*-based MR imaging and its special applications". Radiographics. 29 (5): 1433–49. doi:10.1148/rg.295095034. PMC 2799958. PMID 19755604.
  9. ^ a b Di Muzio B, Gaillard F. "Susceptibility weighted imaging". Retrieved 2017-10-15.
  10. ^ Sharma R, Taghi Niknejad M. "Short tau inversion recovery". Radiopaedia. Retrieved 2017-10-13.
  11. ^ Berger F, de Jonge M, Smithuis R, Maas M. "Stress fractures". Radiology Assistant. Radiology Society of the Netherlands. Retrieved 2017-10-13.
  12. ^ Hacking C, Taghi Niknejad M, et al. "Fluid attenuation inversion recoveryg". radiopaedia.org. Retrieved 2015-12-03.
  13. ^ a b Di Muzio B, Abd Rabou A. "Double inversion recovery sequence". Radiopaedia. Retrieved 2017-10-13.
  14. ^ Lee M, Bashir U. "Diffusion weighted imaging". Radiopaedia. Retrieved 2017-10-13.
  15. ^ Weerakkody Y, Gaillard F. "Ischaemic stroke". Radiopaedia. Retrieved 2017-10-15.
  16. ^ Hammer M. "MRI Physics: Diffusion-Weighted Imaging". XRayPhysics. Retrieved 2017-10-15.
  17. ^ An H, Ford AL, Vo K, Powers WJ, Lee JM, Lin W (May 2011). "Signal evolution and infarction risk for apparent diffusion coefficient lesions in acute ischemic stroke are both time- and perfusion-dependent". Stroke. 42 (5): 1276–81. doi:10.1161/STROKEAHA.110.610501. PMC 3384724. PMID 21454821.
  18. ^ a b Smith D, Bashir U. "Diffusion tensor imaging". Radiopaedia. Retrieved 2017-10-13.
  19. ^ Chua TC, Wen W, Slavin MJ, Sachdev PS (February 2008). "Diffusion tensor imaging in mild cognitive impairment and Alzheimer's disease: a review". Current Opinion in Neurology. 21 (1): 83–92. doi:10.1097/WCO.0b013e3282f4594b. PMID 18180656. S2CID 24731783.
  20. ^ Gaillard F. "Dynamic susceptibility contrast (DSC) MR perfusion". Radiopaedia. Retrieved 2017-10-14.
  21. ^ Chen F, Ni YC (March 2012). "Magnetic resonance diffusion-perfusion mismatch in acute ischemic stroke: An update". World Journal of Radiology. 4 (3): 63–74. doi:10.4329/wjr.v4.i3.63. PMC 3314930. PMID 22468186.
  22. ^ "Arterial spin labeling". University of Michigan. Retrieved 2017-10-27.
  23. ^ Gaillard F. "Arterial spin labelling (ASL) MR perfusion". Radiopaedia. Retrieved 2017-10-15.
  24. ^ Gaillard F. "Dynamic contrast enhanced (DCE) MR perfusion". Radiopaedia. Retrieved 2017-10-15.
  25. ^ Turnbull LW (January 2009). "Dynamic contrast-enhanced MRI in the diagnosis and management of breast cancer". NMR in Biomedicine. 22 (1): 28–39. doi:10.1002/nbm.1273. PMID 18654999. S2CID 5305422.
  26. ^ Chou Ih. "Milestone 19: (1990) Functional MRI". Nature. Retrieved 9 August 2013.
  27. ^ Luijkx T, Gaillard F. "Functional MRI". Radiopaedia. Retrieved 2017-10-16.
  28. ^ a b "Magnetic Resonance Angiography (MRA)". Johns Hopkins Hospital. Retrieved 2017-10-15.
  29. ^ Keshavamurthy J, Ballinger R et al. "Phase contrast imaging". Radiopaedia. Retrieved 2017-10-15.
  30. ^ Le Bihan D; Breton E; Lallemand D; Grenier P; Cabanis E; Laval-Jeantet M (November 1986). "MR imaging of intravoxel incoherent motions: application to diffusion and perfusion in neurologic disorders". Radiology. 161 (2): 401–7. doi:10.1148/radiology.161.2.3763909. PMID 3763909.
  31. ^ "Diffusion Inaging". Stanford University. Archived from the original on 24 December 2011. Retrieved 28 April 2012. {{cite web}}: Unknown parameter |deadurl= ignored (|url-status= suggested) (help)
  32. ^ Filler A (2009). "The History, Development and Impact of Computed Imaging in Neurological Diagnosis and Neurosurgery: CT, MRI, and DTI". Nature Precedings. doi:10.1038/npre.2009.3267.5.
  33. ^ Moseley ME; Cohen Y; Mintorovitch J; Chileuitt L; Shimizu H; Kucharczyk J; Wendland MF; Weinstein PR (May 1990). "Early detection of regional cerebral ischemia in cats: comparison of diffusion- and T2-weighted MRI and spectroscopy". Magn Reson Med. 14 (2): 330–46. doi:10.1002/mrm.1910140218. PMID 2345513.
  34. ^ Wattjes MP; Lutterbey GG; Gieseke J; Träber F; Klotz L; Schmidt S; Schild HH (January 2007). "Double inversion recovery brain imaging at 3T: diagnostic value in the detection of multiple sclerosis lesions". AJNR Am J Neuroradiol. 28 (1): 54–9. PMID 17213424.
  35. ^ Nelson F; Poonawalla AH; Hou P; Huang F; Wolinsky JS; Narayana PA (October 2007). "Improved identification of intracortical lesions in multiple sclerosis with phase-sensitive inversion recovery in combination with fast double inversion recovery MR imaging". AJNR Am J Neuroradiol. 28 (9): 1645–9. doi:10.3174/ajnr.A0645. PMID 17885241.
  36. ^ Nelson F; Poonawalla A; Hou P; Wolinsky JS; Narayana PA (November 2008). "3D MPRAGE improves classification of cortical lesions in multiple sclerosis". Mult. Scler. 14 (9): 1214–9. doi:10.1177/1352458508094644. PMC 2650249. PMID 18952832.
  37. ^ Brant-Zawadzki M; Gillan GD; Nitz WR (March 1992). "MP RAGE: a three-dimensional, T1-weighted, gradient-echo sequence--initial experience in the brain". Radiology. 182 (3): 769–75. doi:10.1148/radiology.182.3.1535892. PMID 1535892.[permanent dead link]
  38. ^ Cite error: The named reference McRobbie was invoked but never defined (see the help page).
  39. ^ Wheaton AJ; Miyazaki M (2012). "Non-contrast enhanced MR angiography: physical principles". J Magn Reson Imaging. 36 (2): 286–304. doi:10.1002/jmri.23641. PMID 22807222.
  40. ^ Filippi M; Rocca MA; De Stefano N, Enzinger C; Fisher E; Horsfield MA; Inglese M; Pelletier D; Comi G (2011). "Magnetic Resonance Techniques in Multiple Sclerosis". Archives of Neurology. 68 (12): 1514–20. doi:10.1001/archneurol.2011.914. ISSN 0003-9942. PMID 22159052.
  41. ^ Borthakur A; Mellon E; Niyogi S; Witschey W; Kneeland JB; Reddy R (November 2006). "Sodium and T1rho MRI for molecular and diagnostic imaging of articular cartilage". NMR Biomed. 19 (7): 781–821. doi:10.1002/nbm.1102. PMC 2896046. PMID 17075961.
  42. ^ a b "Structural MRI Imaging". UC San Diego School of Medicine. Retrieved 2017-01-01.
  43. ^ De Coene B; Hajnal JV; Gatehouse P; Longmore DB; White SJ; Oatridge A; Pennock JM; Young IR; Bydder GM (1992). "MR of the brain using fluid-attenuated inversion recovery (FLAIR) pulse sequences". AJNR Am J Neuroradiol. 13 (6): 1555–64. PMID 1332459.
  44. ^ Wiggermann C; Hernandez-Torres E; Vavasour I; Moore W; Laule C; MacKay A; Li D; Traboulsee A; Rauscher A (June 2013). "Magnetic resonance frequency shifts during acute MS lesion formation". Neurology. 81 (3): 211–218. doi:10.1212/WNL.0b013e31829bfd63. PMC 3770162. PMID 23761621.
  45. ^ Reichenbach JR; Venkatesan R; Schillinger DJ; Kido DK; Haacke EM (July 1997). "Small vessels in the human brain: MR venography with deoxyhemoglobin as an intrinsic contrast agent". Radiology. 204 (1): 272–7. doi:10.1148/radiology.204.1.9205259. PMID 9205259.[permanent dead link]
  46. ^ page 64 in: Dominik Weishaupt, Victor D. Köchli, Borut Marincek (2008). How does MRI work?: An Introduction to the Physics and Function of Magnetic Resonance Imaging (2 ed.). Springer Science & Business Media. ISBN 9783540378457.{{cite book}}: CS1 maint: multiple names: authors list (link)
  47. ^ Richard Gore and Robin Smithuis (2014-05-21). "Bowel wall thickening - CT-pattern - Type 4 - Fat target sign". Radiology Assistant. Retrieved 2017-09-27.
  48. ^ Page 70 in: Dominik Weishaupt, Victor D. Koechli, Borut Marincek (2008). How does MRI work?: An Introduction to the Physics and Function of Magnetic Resonance Imaging (2 ed.). Springer Science & Business Media. ISBN 9783540378457.{{cite book}}: CS1 maint: multiple names: authors list (link)
  49. ^ Sasaki M; Shibata E; Tohyama K; Takahashi J; Otsuka K; Tsuchiya K; Takahashi S; Ehara S; Terayama Y; Sakai A (July 2006). "Neuromelanin magnetic resonance imaging of locus ceruleus and substantia nigra in Parkinson's disease". NeuroReport. 17 (11): 1215–8. doi:10.1097/01.wnr.0000227984.84927.a7. PMID 16837857.