Liangjie Lin1, Yanqin Lin1, Zhiliang Wei1, and Zhong Chen1
1Electronic science, Xiamen University, Xiamen, China, People's Republic of
Synopsis
Magnetic resonance spectroscopy (MRS) is a
powerful noninvasive tool in diagnoses, progressive monitoring, and studies of
disease states of humans and animals. In this study, we present a MRS pulse
sequence for localized one-dimensional in-phase proton MRS. The proposed pulse
sequence can be utilized to reduce undesired broad resonances with short T2s
and increasing signal intensity of J
coupling metabolites. Moreover, it provides an approach of direct measurement
of non-overlapping J coupling peaks
at achievable arbitrary TEs and of their transverse relaxation times (T2).PURPOSE
Magnetic resonance spectroscopy (MRS) is a
powerful noninvasive tool in diagnoses, progressive monitoring, and studies of
disease states of humans and animals. Point resolved spectroscopy (PRESS) and the
stimulated echo acquisition mode (STEAM) technique have been extensively used
to acquire localized one dimensional (1D)
1H MRS. However, both
PRESS and STEAM sequences, especially when they are performed with long echo
times (TEs), can suffer from
J
modulations during TEs. In the Carr Purcell-selected PRESS (CPRESS) experiment,
1 J modulations can be
suppressed through quick repeating 180 pulses with short interpulse intervals at
the cost of high radio frequency (RF) power deposition. In this study, we
propose a modified pulse sequence called IP-PRESS for in-phase point resolved
spectroscopy.
METHODS
The schematic diagram of the IP-PRESS sequence is
shown in Fig. 1. It starts with a 90º excitation pulse, and
then follows with N repeated J-refocused
modules which employ a 90º pulse at the
midpoint of a double spin echoes. These repeated J-refocused modules are necessary for keeping J modulations suppressed at moderate or long TEs. The J-refocused module before acquisition, consisting
of selective pulses along with slice selection and spoiler gradients along
three orthogonal axes, is capable of achieving 3D spatial localization in one
shot. In comparison with the standard PRESS sequence, additional pulses are
employed by IP-PRESS sequence, especially at long TEs, resulting in increased RF
power deposition. For suppressing J
modulations, the interpulse intervals (τ1
and τ2) need to meet the requirement of τ << 1/J which
can be much easier to reach in comparison with demands in the CPMG type
sequences. 2
A sample
of ethyl 3-bromopropionate (0.5M in CDCl3) was utilized to test the performance of the IP-PRESS
sequence. The voxel size was 4.0×4.0×16.0 mm3, and the repetition time
was 4 s with no average. The interpulse intervals were set as τ1 = τ2 = 5 ms, and
repetition number N were varied to obtain TEs from 20 to 500 ms with a step
size of 20 ms. All experiments were
performed on an 11.7 T Varian NMR System (Agilent Technologies, Santa Clara,
CA, USA) with a 54 mm narrow bore, using a 5-mm indirect detection probe of 1.6
cm effective length at 298 K.
RESULTS
The IP-PRESS spectra of ethyl 3-bromopropionate
are shown in Fig. 2a. Spectral peaks in IP-PRESS spectra almost keep in-phase
with varied TEs. It suggests that
J coupling modulations can be suppressed with IP-PRESS at achievable
arbitrary echo times (TE). For typical
metabolite T2 measurements, a series of MRS spectra are acquired with varying
TEs. The signal intensities are quantified, and then used for exponential
decaying fitting to obtain T2 values. With conventional MRS sequences, such as
PRESS, signal intensities and phases of coupled resonances are modulated by
J couplings with varying TEs, and thus
signal quantification from acquired spectra cannot directly be used for
exponential fitting. The IP-PRESS sequence suppresses
J modulations at arbitrary TEs (see Fig. 2b), providing an approach
for direct quantification and exponential fitting for scalar coupled peaks from
acquired spectra.
CONCLUSION
In conclusion, the acquired IP-PRESS
in-phase spectra are beneficial for reducing undesired broad resonances with
short T2s at medium/long TEs and increasing signal intensities for
J coupling metabolites. Moreover, they
provide an approach of direct measurement of non-overlapping
J coupling peaks at achievable arbitrary
TEs and of their transverse relaxation times (T2).
Acknowledgements
This work was partially supported by the
National Natural Science Foundation of China under Grants 11105114 and
11375147, and the Natural Science Foundation of Fujian Province of China under
Grant 2014J05012. The authors thank Dr. Jianghua Feng for helpful discussion
during the course of this work.References
1. Hennig J, Thiel T, Speck O. Improved sensitivity
to overlapping multiplet signals in in vivo proton spectroscopy using a
multiecho volume selective (CPRESS) experiment. Magn Reson Med
1997;37(6):816-820.
2. Aguilar JA, Nilsson M, Bodenhausen G, Morris GA.
Spin echo NMR spectra without J modulation. Chem Commun 2012;48(6):811-813.