DOI:10.2214/AJR.06.0567
AJR 2007; 188:919-926
© American Roentgen Ray Society
Semiquantitative Assessment of First-Pass Renal Perfusion at 1.5 T: Comparison of 2D Saturation Recovery Sequences With and Without Parallel Imaging
Henrik J. Michaely1,
Harald Kramer1,
Niels Oesingmann2,
Klaus-Peter Lodemann3,
Maximilian F. Reiser1 and
Stefan O. Schoenberg1
1 Department of Clinical Radiology, University of Munich, Grosshadern-Campus,
Marchionistrasse 15, Munich, Germany, 81377.
2 Siemens Medical Solutions, Malvern, PA.
3 Bracco-Altana Pharma, Konstanz, Germany.
Received April 26, 2006;
accepted after revision August 31, 2006.
Address correspondence to H. J. Michaely
(henrik.michaely{at}med.uni-muenchen.de).
Sponsored through a grant from Bracco-Altana Pharma, Konstanz, Germany.
The employment of N. Oesingmann at Siemens Medical Solutions and K. P.
Lodemann at Bracco-Altana Pharma did not influence the data in this study.
Abstract
OBJECTIVE. The purpose of this study was to assess the feasibility
and reliability of measurements performed with true fast imaging with
steady-state free precession (FISP) and turbo fast low-angle shot (FLASH)
sequences with parallel imaging compared with those obtained with turbo FLASH
sequences without parallel imaging in first-pass renal perfusion MRI.
SUBJECTS AND METHODS. The subjects in this prospective study were 15
healthy men who volunteered to undergo MRI for acquisition of renal perfusion
measurements. Imaging was performed at 1.5 T with the following three
techniques after administration of gadobenate dimeglumine at 4 mL/s:
saturation recovery (SR) turbo FLASH sequences without parallel imaging, SR
turbo FLASH sequences with parallel imaging, and SR true FISP sequences. The
spatial resolution was 2.3 x 2.6 x 8 mm with a temporal resolution
of four slices per second (turbo FLASH without parallel imaging and true FISP)
or six slices per second (turbo FLASH with parallel imaging). The
semiquantitative perfusion parameters mean transit time and maximal upslope
were determined. Signal-to-noise ratio (SNR), delta ratio, and time to maximal
signal intensity also were determined. Image quality was rated in
consensus.
RESULTS. Image quality was best for turbo FLASH sequences without
parallel imaging compared with true FISP and turbo FLASH sequences with
parallel imaging. True FISP sequences yielded the highest baseline SNR (26.7)
but the lowest delta ratio (3.2). Turbo FLASH sequences without and with
parallel imaging had significantly lower SNRs (9.6 and 9.3) and significantly
higher delta ratios (5.1 and 5.0). The first-pass perfusion parameters mean
transit time and time to maximal signal intensity were independent of the
technique used.
CONCLUSION. It seems that at 1.5 T, turbo FLASH sequences without
parallel imaging are the best approach to renal first-pass perfusion
imaging.
Keywords: genitourinary tract imaging kidney MRI technique perfusion-weighted MRI renal perfusion
Introduction
Despite technical advances, diagnosis of renovascular hypertension
with MR angiography remains a challenge
[1]. Therefore, additional
dynamic, first-pass imaging with gadolinium enhancement is being used
increasingly to assess organ perfusion in patients with suspected renal artery
stenosis [2]. The clinical
importance of perfusion measurements is emphasized by the fact that reduced
renal perfusion is associated with increased morbidity and mortality
[3,
4]. In previous studies,
various imaging techniques, such as multiphasic T1-weighted sequences
[2,
5,
6] and volume-inter-polated
breath-hold examination sequences
[7], have been used. Both
approaches are based on spoiled gradient-echo sequences. Fast low-angle shot
(FLASH) sequences, particularly turbo FLASH sequences, which are characterized
by an additional magnetization preparation, are known to show a high degree of
linearity between signal intensity and gadolinium concentration
[8,
9]. These sequences are robust,
fast, and not prone to specific absorption rate (SAR) restrictions; they do,
however, have a moderate signal-to-noise-ratio (SNR)
[10].
Compared with renal perfusion imaging, cardiac perfusion imaging has become
established as a standard clinical tool
[11]. In cardiac imaging, fast
imaging with steady-state free precession (FISP) sequences, such as true FISP,
have become standard because they have a higher inherent SNR than turbo FLASH
sequences [12,
13]. Parallel imaging,
introduced to perfusion imaging to improve temporal resolution and to increase
the number of slices simultaneously acquired
[14], is considered standard
technique for cardiac perfusion imaging.
The aim of this intraindividual comparison study was twofold. The first
goal was to compare the feasibility and reliability of true FISP renal
first-pass perfusion imaging with those of a turbo FLASH sequence, the
standard of reference. The second aim was to assess the feasibility and value
of parallel imaging in measurement of renal perfusion.
Subjects and Methods
Study Concept
The aim of this prospective, intraindividual comparison study was to
investigate the best sequence for renal perfusion measurements. Fifteen
healthy male volunteers underwent renal perfusion measurements on three
different days with a different imaging sequence on each day. The sequences
were saturation recovery (SR) turbo FLASH without parallel imaging, SR true
FISP, and SR turbo FLASH with parallel imaging. Because, to our knowledge, all
published data on renal perfusion have been obtained with fast spoiled
gradient-echo sequences, the turbo FLASH sequence without parallel imaging was
considered the standard of reference against which a true FISP sequence
without parallel imaging and a turbo FLASH sequence with a parallel imaging
acceleration factor of 2 were tested.
Subjects
After internal review board approval was granted, informed consent was
obtained from 15 healthy men who volunteered for the study. The subjects were
25-38 years old (mean age, 29.1 ± 3.1 years) and had no history of
renal or vascular disease. Because of internal review board restrictions, only
men were eligible for this study. All volunteers were well hydrated at the
time of the examinations. Vital signs were checked before imaging and 10
minutes after the volunteers left the MRI machine. A 20-gauge needle was
placed in an antecubital vein of all volunteers for administration of the
contrast agent. For each examination, a blood sample was drawn from each
volunteer and analyzed in the hospital laboratory to measure serum creatinine
level to rule out previously unknown renal disease.
MRI
Measurements were performed on a 32-channel 1.5-T whole-body MRI unit
(Magnetom Avanto, 76 x 32, Siemens Medical Solutions) with a gradient
strength of 45 mT/m and slew rate of 200 mT/m/ms. For signal reception, one
body matrix with six independent receiver elements and six elements of the
spine matrix were usedthat is, a total of 12 independent receiver
elements. Before perfusion imaging, true FISP sequences in the coronal and
transverse orientations were acquired for proper positioning. The following
three sequences for measurement of renal perfusion were used on the three
examination days, which were separated by at least 1 day and an average of 3
days: day 1, SR turbo FLASH sequence without parallel imaging and with MR
angiography; day 2, SR true FISP; day 3, SR turbo FLASH with parallel
imaging.
The parameters for all sequences are shown in
Table 1. The slices of the
perfusion measurement sequences were positioned in an oblique coronal
orientation over the kidneys with a single slice in an axial orientation
through the kidneys.
All sequences were performed with the SR technique, which grants complete
and homogeneous saturation over the entire selected imaging volume and thereby
minimizes inflow-related artifacts. For magnetization preparation, a pulse
train of three short
/2 pulses with constant amplitude and phase cycling
in a phase angle of
/2 was applied. The pulse train was followed by a
10-mT/m spoiler over 1 millisecond. More than three pulses did not
significantly improve the saturation effect but lengthened the preparation
phase. The time between the preparation pulses and acquisition of the central
image line (inversion time) is given in
Table 1.
For the turbo FLASH sequences without parallel imaging, a linear relation
between contrast medium concentration and signal intensity for a wide range of
concentrations up to 1.1 mmol/L is well known
[8]. A standardized contrast
bolus of 7 mL of gadobenate dimeglumine (MultiHance, Bracco Pharma) was
injected into an antecubital vein at a flow rate of 4 mL/s for the perfusion
measurements and was followed by 30 mL of saline solution. Owing to weak
protein binding, gadobenate dimeglumine has higher relaxivity than
conventional gadolinium chelates
[15] and therefore yields
stronger enhancement.
For two reasons, contrast agent injection was started simultaneously with
the start of the imaging sequences. First, magnetization is driven into the
steady state before arrival of contrast agent in the kidney; second,
unenhanced images are needed for successful postprocessing. The volunteers
were instructed to hold their breath as long as possible to allow motion-free
monitoring of the first pass of the contrast agent.
A phantom containing eight vials (2 x 11 cm) of albumin-gadobenate
dimeglumine solution was placed under the volunteers. The vials had the
following increasing concentrations of gadobenate dimeglumine: 0.03125, 0.125,
0.25, 0.5, 1, 4, 8, and 16 mmol/L. The phantom was tempered to 37°C. The
axial slice of the perfusion sequence was positioned to include the phantom
(Fig. 1A,
1B,
1C).

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Fig. 1B 28-year-old man in good health. Graph shows measured mean
peak signal intensities in aorta and both kidneys. True fast imaging with
steady-state free precession (FISP) sequence yields highest absolute signal
from enhanced kidneys and enhanced aorta. Turbo FLASH sequences with and
without parallel imaging (PI) perform in similar way. AU = arbitrary
units.
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Fig. 1C 28-year-old man in good health. Graph shows calibration curve
with measured signal intensities from first five vials (0.032-1.0 mmol/L of
gadobenate dimeglumine). Peak signal intensity measured in aorta and kidneys
(B) are well within increasing part of calibration curve.
T2*-related loss of signal intensity can therefore safely be ruled
out. Solid line indicates regression for true FISP sequence; dashed line,
regression for turbo FLASH sequence; dotted line, regression for turbo FLASH
sequence with parallel imaging.
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During the first examination, contrast-enhanced MR angiography was
performed to rule out renal artery stenosis. To allow the contrast agent to
leave the vessel bed, the examination was stopped for at least 5 minutes after
initial contrast administration. A test bolus technique was used to determine
circulation time. A full 3D MR angiographic data set (spatial resolution, 1.0
x 0.8 x 1.0 mm; generalized autocalibrating partially parallel
acquisition [16]; parallel
imaging acceleration factor, 3; acquisition time, 19 seconds) was acquired.
For MR angiography, a standardized 20-mL bolus of gadobenate dimeglumine was
injected into an antecubital vein at a flow rate of 2 mL/s and was followed by
a 30-mL saline chaser administered at 2 mL/s.
Perfusion Data Analysis
MR perfusion measurements were analyzed on an offline workstation with MERZ
software (version 0.99, Siemens Medical Solutions)
[2]. According to this
software, region of interest (ROI)-based evaluation of contrast enhancement on
a pixel-by-pixel basis yields a signal intensity-time curve. The sizes of the
ROIs were chosen to include at least 400 pixels. The ROIs were positioned over
the renal cortex, sparing the surrounding fat and renal medulla.
Figure 2 shows positioning in
the ROI. The ROIs were automatically corrected for motion. This motion
correction algorithm is based on a next-neighbor approach.
MERZ operates with a Marquardt-Levenberg least squares
[17] algorithm for automatic
acquisition of a gamma variate fit
[18] of the initial signal
intensity-time curve. If desired, it is possible to interact with the fitting
process by confining the time intervals and parameters for finding reasonable
start values. Goodness of fit is presented after successful fitting. Examples
of signal intensity-time curves and the derived fitted curves for all three
techniques are shown in Figure
3A,
3B. The gamma variate fit
founded on the indicator dilution theory describes the first-pass component of
tracer kinetics and has been used for description of renal blood flow in
imaging techniques such as CT and electron beam tomography
[19,
20].

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Fig. 3A 25-year-old man in good health. Signal intensity-time curves
for three MRI sequences. Dotted lines indicate true fast imaging with
steady-state free precession (FISP), solid gray lines indicate turbo fast
low-angle shot (FLASH) without parallel imaging, and solid black lines
indicate turbo FLASH with parallel imaging. Graph shows marked differences in
configuration of first pass peak. AU = arbitrary units.
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Fig. 3B 25-year-old man in good health. Signal intensity-time curves
for three MRI sequences. Dotted lines indicate true fast imaging with
steady-state free precession (FISP), solid gray lines indicate turbo fast
low-angle shot (FLASH) without parallel imaging, and solid black lines
indicate turbo FLASH with parallel imaging. Gamma variate fit of curves in
A. True FISP sequence yielded lowest maximal signal intensity and
slowest upslope of curve. Mean transit time and time to peak were equal for
all techniques. Scale of x-axis is slightly different from that in
A.
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The four following characteristic curve parameters can be derived from the
gamma variate fit: time to maximal signal intensity, maximal upslope (ds/dt),
maximal signal intensity (baseline corrected), and first moment of function
that corresponds to the mean transit time of the tracer. To compensate for
intraobserver variability, the mean values of two ROIs were used for further
analysis.
SNR Measurements
The signal intensity of the eight vials of the phantom was measured for
each volunteer and plotted against concentration. Because dynamic imaging
always represents a problem for objective SNR measurements, a previously
described [21] difference
method was used for all sequences. This method eliminates the problem of
inhomogeneous distribution of noise. Two baseline images obtained before
arrival of contrast agent in the kidney were subtracted. The mean SD of an ROI
drawn in the region of the kidneys was used as image noise. To avoid
saturation-related artifacts, the first four images were not used for image
noise calculation. Signal intensity for the baseline SNR calculation was
measured as the mean value of an ROI over the unenhanced kidneys and the
aorta. For peak SNR calculation, ROIs were placed over the aorta and kidneys
at the point of maximal enhancement, and mean signal intensity again was
measured. Baseline and peak SNRs were calculated as follows:
 |
To compare the relative enhancement between baseline SNR and peak SNR, the
delta ratio was computed for the kidney and aorta as follows:
Visual Assessment
The image quality of the perfusion sequences was rated by two radiologists
in consensus. Overall image quality was based on the presence and degree of
artifacts and on demarcation of the kidney from the surrounding tissue. An
ordinal scale with three grades was used: 1, no artifacts, kidneys easily
differentiated from the surrounding tissues; 2, visible artifacts, kidneys
easily differentiated from the surrounding tissues or no artifacts but kidneys
difficult to differentiate from surrounding tissues; 3, visible artifacts and
kidneys difficult to differentiate from surrounding tissues.
Statistical Analysis
All values are mean and SD. Results of the Kolmogorov-Smirnov test proved
that the data followed gaussian distribution. For that reason, Student's
t tests were used for further comparison. Without correction there
would be a 46.0% chance of finding one or more significant differences in the
12 tests performed. Therefore, Bonferroni correction
[22] for multiple comparisons
was performed and resulted in a significance level of p < 0.0042.
For comparison of perfusion parameters, the SR turbo FLASH sequence was
considered the standard of reference. The median was used to describe the
visual assessment data. All statistical analyses were performed with SPSS
version 12.0.1 software (SPSS, Inc.).
Results
The perfusion measurements were obtained without problems in all
volunteers. No adverse effects occurred. The additional MR angiography did not
reveal renal artery disease. Serum creatinine levels were within normal limits
for all volunteers on all examination days (mean serum creatinine
concentration, 1.1 ± 0.1 mg/dL).
Measurement of peak signal intensity revealed a peak in the kidneys of 56.7
± 26.4 arbitrary units (AU) for the turbo FLASH sequence with parallel
imaging, 60.1 ± 25.0 AU for turbo FLASH without parallel imaging, and
109.2 ± 20.5 AU for true FISP. In the aorta, peak signal intensity was
104.0 ± 17.8 AU for turbo FLASH with parallel imaging, 94.0 ±
19.9 AU for turbo FLASH without parallel imaging, and 189.9 ± 49.5 AU
for true FISP. As Figure 1A,
1B,
1C shows, these values were
within the rising part of the calibration curve. T2*-related
alteration of measured signal intensity therefore was ruled out. A similar
result was found for SNR, which was significantly (p < 0.0001)
higher for true FISP in unenhanced kidney, enhanced kidney, and the aorta
(Fig. 4A,
4B). In contrast, the delta
ratio, which describes relative enhancement normalized to baseline SNR, was
significantly lower for the true FISP (3.2 ± 0.8) sequence compared
with the turbo FLASH sequences with (5.1 ± 1.1) and without (5.0
± 2.2) parallel imaging (Fig.
3A,
3B).

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Fig. 4A Comparison of sequences. Graph shows comparison of measured
signal-to-noise ratio (SNR) at baseline and peak enhancement in renal cortex
and abdominal aorta. True fast imaging with steady-state free precession
(FISP) sequence yields highest SNR. Turbo fast low-angle shot (FLASH)
sequences with and without parallel imaging (PI) behave similarly to each
other.
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Fig. 4B Comparison of sequences. Graph shows delta ratio comparisons
for three sequences. True FISP yielded highest SNR at baseline and during peak
enhancement. Relative enhancementthat is, delta ratiohowever,
was only 3.2 for true FISP. Turbo FLASH sequences had 59% higher delta ratios
of 5.1 with and 5.0 without parallel imaging.
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The exact values of the semiquantitative perfusion parameters with mean and
SD are shown in Table 2. Almost
equal values for mean transit time of approximately 14.8 seconds and time to
maximal signal intensity of approximately 11.1 seconds were found for all
three sequences. For maximal signal intensity, no significant difference was
found between the turbo FLASH sequences with and without parallel imaging. The
maximal upslope of the signal intensity-time curve also showed no significant
differences between these two sequences. In contrast, the true FISP sequence
had statistically significantly (p < 0.00002) lower maximal signal
intensity and maximal upslope than the turbo FLASH sequences with and without
parallel imaging.
Examples of image quality are shown in Figure
5A,
5B,
5C,
5D,
5E,
5F,
5G,
5H,
5I. Visual assessment of image
quality yielded the highest rating for the turbo FLASH sequence without
parallel imaging, a median of 1. Both true FISP and turbo FLASH with parallel
imaging were given a median rating of 2. True FISP was rated lower because it
yielded lower relative signal enhancement after contrast administration, weak
contrast between the kidneys and perirenal fat tissue, susceptibility
artifacts, and banding artifacts. The turbo FLASH sequence with parallel
imaging suffered from increased, perceivable image noise and reconstruction
artifacts, which became especially visible after first-pass perfusion (Fig.
6A,
6B,
6C,
6D). The kidneys became very
difficult to differentiate with turbo FLASH sequences without parallel imaging
in the late phase of perfusion, in which most of the contrast agent had left
the vascular system.

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Fig. 5D 29-year-old man in good health. Unenhanced (D), early
arterial phase (E), and medullary phase (F) MR images obtained
with turbo FLASH sequence with parallel imaging show higher noise level than
A-C.
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Fig. 5E 29-year-old man in good health. Unenhanced (D), early
arterial phase (E), and medullary phase (F) MR images obtained
with turbo FLASH sequence with parallel imaging show higher noise level than
A-C.
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Fig. 5F 29-year-old man in good health. Unenhanced (D), early
arterial phase (E), and medullary phase (F) MR images obtained
with turbo FLASH sequence with parallel imaging show higher noise level than
A-C.
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Fig. 5G 29-year-old man in good health. Unenhanced (G), early
arterial phase (H), and medullary phase (I) MR images obtained
with true fast imaging with steady-state free precession sequence yield best
signal-to-noise ratio, but because of higher background signal intensity,
kidneys are difficult to differentiate.
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Fig. 5H 29-year-old man in good health. Unenhanced (G), early
arterial phase (H), and medullary phase (I) MR images obtained
with true fast imaging with steady-state free precession sequence yield best
signal-to-noise ratio, but because of higher background signal intensity,
kidneys are difficult to differentiate.
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Fig. 5I 29-year-old man in good health. Unenhanced (G), early
arterial phase (H), and medullary phase (I) MR images obtained
with true fast imaging with steady-state free precession sequence yield best
signal-to-noise ratio, but because of higher background signal intensity,
kidneys are difficult to differentiate.
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Fig. 6A 29-year-old man in good health. MR image obtained with single
true fast imaging with steady-state free precession sequence shows
susceptibility artifacts that occur when kidney is close to air-filled large
bowel. Margins of renal cortex (arrows) are not clearly defined on
either side.
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Fig. 6B 29-year-old man in good health. Medullary phase (D) MR
images obtained with turbo fast low-angle shot sequence with parallel imaging
show typical bandlike reconstruction artifact (arrows). Artifacts
were seen especially in late phases of perfusion measurement after
intravascular concentration of contrast agent had markedly decreased.
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Fig. 6C 29-year-old man in good health. Medullary phase (D) MR
images obtained with turbo fast low-angle shot sequence with parallel imaging
show typical bandlike reconstruction artifact (arrows). Artifacts
were seen especially in late phases of perfusion measurement after
intravascular concentration of contrast agent had markedly decreased.
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Fig. 6D 29-year-old man in good health. Medullary phase (D) MR
images obtained with turbo fast low-angle shot sequence with parallel imaging
show typical bandlike reconstruction artifact (arrows). Artifacts
were seen especially in late phases of perfusion measurement after
intravascular concentration of contrast agent had markedly decreased.
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Discussion
The main focus of this study was to evaluate the value of true FISP and
turbo FLASH sequences in first-pass renal perfusion at 1.5 T. The results
study shows that for assessment of first-pass renal perfusion, turbo FLASH
without parallel imaging appears to be a better sequence than true FISP and
turbo FLASH with parallel imaging. The parameters' mean transit time and time
to maximal signal intensity were found equal for all techniques used. In
another study [23], these
parameters were also found equal for measurements with a time-resolved
angiographic technique with high temporal resolution at 3.0 T. In contrast,
the maximum upslope and maximal signal intensity were significantly different
between the turbo FLASH sequences and the true FISP sequence. With equal time
to maximum signal intensity, higher maximum signal intensity automatically
leads to increased maximum upslope.
The results may seem confusing in light of the SNR values, the highest
measured signal intensity and SNR values being found for the true FISP
sequence. The solution to this paradox lies in the postprocessing program
MERZ, which performs a baseline correction during the fitting and yields
signal intensity values normalized to the unenhanced images. A closer look at
the delta ratio confirms these conclusions. The delta ratio of the kidneys,
the relative enhancement rate, was 38% lower with true FISP than with turbo
FLASH sequences. This result may be a consequence of the mixed contrast
behavior of true FISP, which is determined by T1 and T2 weighting
[24], whereas turbo FLASH
sequences are heavily T1 weighted
[25]. As a consequence,
unenhanced true FISP images reveal higher baseline signal intensity in the
kidney because of high renal water content. In contrast, true FISP has shown
the greatest enhancement in myocardial perfusion studies
[13]. This contradiction can
be explained in the same way as for renal studies. The myocardium shows only
little signal intensity without contrast material but is highly vascularized
and shows strong enhancement.
In our study, the weaker peak arterial contrast enhancement was one reason
the true FISP images were scored worse than the turbo FLASH images. In
addition to weak relative enhancement, the true FISP images often had banding
and susceptibility artifacts. Although they did not hinder assessment of renal
perfusion in this study, these artifacts can be troublesome if air-filled
large bowel is adjacent to the kidneys and if higher field strengths are used
[26]. In addition, because of
the high intrinsic SNR of true FISP sequences
[27,
28] and the high fat content,
differentiating enhanced kidney from perinephric fat was more difficult with
true FISP than with turbo FLASH sequences.
The high signal intensity of the kidneys with true FISP can be explained by
the mixed contrast behavior of steady-state free precession, which depends on
T2 and T1 weighting. Therefore, the low T1 relaxation time of water does not
necessarily lead to a lower SNR. Images obtained with the turbo FLASH sequence
with parallel imaging were scored equally as low as true FISP images, but for
another reason. Even though the SNR of turbo FLASH with parallel imaging was
lower at baseline than the SNR of turbo FLASH without parallel imaging, the
peak arterial enhancement for turbo FLASH with parallel imaging was the
highest of all three sequences investigated. In the late phases, which are
used to determine renal excretory function, it became very difficult to
differentiate kidney from surrounding tissues with use of turbo FLASH with
parallel imaging.
Use of parallel imaging produced artifacts, which were mainly seen after
the main fraction of contrast material had left the vessel bed. These
artifacts were particularly pronounced in the image noise and were present to
a lesser extent in the spleen and kidneys. The use of newer parallel imaging
reconstruction algorithms, such as temporal sensitivity encoding
[29], may reduce these
artifacts in the future. Temporal sensitivity encoding also may be more
suitable than the generalized autocalibrating partially parallel acquisition
algorithm for dynamic measurements because temporal sensitivity encoding
obviates acquisition of reference lines and hence allows faster imaging with a
higher temporal resolution
[29]. Initial results in
cardiac functional cine studies have proved acceleration factors of 4 to be
feasible at 1.5 T [21].
Overall, our results imply that maximal upslope and maximal signal
intensity seem to vary with the technique used and that mean transit time and
time to maximal signal intensity seem to be independent of field strength.
Maximal upslope has often been reported as a sensitive marker for perfusion
deficits [6,
9]. However, in view of our
results, care should be taken when maximal upslope values are compared.
This study was designed as a volunteer comparison study. Because the
results are promising, patient studies should be undertaken to evaluate
perfusion abnormalities in renal parenchymal and vascular diseases. In this
context, determination of segmental contrast-to-noise changes, as in segmental
renal transplant dysfunction or accessory renal artery stenosis, should be
valuable in defining extent of disease.
In view of our results, future studies with turbo FLASH sequences are
likely to profit from transition to 3.0 T in terms of increased image quality.
A turbo FLASH sequence that spoils all remaining transverse magnetization
after each readout is prone to neither increased susceptibility nor specific
absorption rate limitations at 3.0 T. Higher field strength may allow use of
parallel imaging with less SNR penalty and fewer artifacts than at 1.5 T. It
also may be possible to use increased SNR at higher field strength to increase
spatial resolution with less SNR penalty and less deterioration of image
quality. In contrast, because of enhanced susceptibility and the problem of
the high specific absorption rate from radiofrequency deposition with
steady-state free precession sequences, such as true FISP, use of a true FISP
sequence for renal perfusion measurements theoretically is less advantageous
at 3.0 T.
A potential limitation of this study was that all volunteers were given a
7-mL bolus of contrast agent. A separate study of optimal contrast agent dose
would be desirable. Assessment of contrast dose was not one of the aims of our
investigation.
In conclusion, this study showed that first-pass renal perfusion
measurements with a true FISP sequence and a turbo FLASH sequence with
parallel imaging are feasible and have equal results for mean transit time and
time to maximal signal intensity. Maximal upslope and maximal signal intensity
were significantly different between the turbo FLASH sequences with and
without parallel imaging and the true FISP sequence. In contrast to myocardial
perfusion measurements, renal perfusion measurements with true FISP sequences
do not seem favorable because of the 38% lower delta ratio compared with that
of turbo FLASH sequences. Use of parallel imaging allows coverage of more
slices simultaneously but at the cost of image quality. Therefore, because of
advantageous contrast behavior and the absence of artifacts, SR turbo FLASH
without parallel imaging appears to be the most appropriate sequence for
assessment of first-pass renal perfusion at 1.5 T.
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