Historical Information

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Older methods and literature references will go here...

Extra section to be removed

Bottomley PA. Spatial localization in NMR spectroscopy in vivo. Ann NY Acad Sci 1987;508:333–48 https://doi.org/10.1111/j.1749-6632.1987.tb32915.x

PRESS1
PRESS2


PRESS Broadband

The product refocusing pulses within PRESS can be replaced by broadband refocusing pulses described in M. Janich et al., Slice-selective broadband refocusing pulses for the robust generation of crushed spin-echoes, J Magn Reson, 223: 129 – 137 (2012) https://doi.org/10.1016/j.jmr.2012.08.003 to reduce the CSDE.

PRESS-Broadband-1
PRESS-Broadband-2

CV 0 5000

CV0: spectral width The total spectral frequency width in Hz.


CV 1 4096

CV1: number of points The number of complex data points acquired per excitation.


CV 4 128 (1.5T) 64 (3T)

CV4: total number of scans The total number of excitations acquired per echo (cycle) when signal averaging. The value of CV4 must be an integer multiple of NEX.


CV 14 0

CV14: JPRESS Mode

0 (PRESS) standard PRESS acquisition, TE1 is set by sequence to minimum

1 (asym. PRESS) TE1 is set by user

2 (half-echo) standard JPRESS acquisition mode, echo acquired from echo top

3 (max-echo) maximum-echo mode described in [6]. For shortest echo time echo is acquired from echo top, for longer echo times data acquisition starts before the echo top.


CV 18 7

CV18: ROI edge sat/gradient mask There are three pairs of VSS RF pulses available at the edge of the Spectroscopy VOI. The VSS can be selected or deselected.

0 – no VSS RF pulses;

1 – S/I the superior and inferior pulses only;

2 – A/P the anterior and posterior pulses only;

3 – S/I and A/P, two pulse pairs;

4 – R/L the right and the left pulses only;

5 – R/L and S/I, two pulse pairs;

6 - R/L and A/P, two pulse pairs;

7 – R/L, A/P and S/I, three pulse pairs, this is the default value

This bitmask determines the polarity of the slice gradients of the three PRESS excitation/refocusing pulses and therefore the direction of the fat-water chemical shift. The corresponding bit set to 1 is negative polarity, 0 is positive.

0 – S/I, A/P and R/L all positive, this is the default value

8 – S/I negative, A/P and R/L positive

16 – A/P negative, S/I and R/L positive

24 – S/I and A/P negative, R/L positive

32 – R/L negative, S/I and A/P positive

40 – R/L and S/I negative, A/P positive

48 - R/L and A/P negative, S/I positive

56 – R/L, A/P and S/I all negative


CV 23 20

CV23: Refocusing Pulse Shape: PRESS refocusing pulse shape

20 – S-BREBOP-7500.rho, pw = 7.5ms

26 – flip_1803.rho, non-linear phase refocusing pulse used for CPRESS

-1 – default pulse set by PSD


CV 24 1

CV24: Feature flag

1 (no add) Store each single data acquisition in pfile.

2 (Bloch-Siegert) Bloch-Siegert TG calibration




PRESS FatSat

The dual BASING technique can be used for additional metabolite suppression, e.g. fat.

J. Star-Lack et al., Improved Water and Lipid Suppression for 3D PRESS CSI Using RF Band Selective Inversion with Gradient Dephasing (BASING), Magn Reson Med, 38, 311 – 321, (1997) https://doi.org/10.1002/mrm.1910380222


CPRESS

CPRESS is a modified PRESS spectroscopic localization pulse sequence that replaces each of the two refocusing RF pulses with a pair of non-linear phase refocusing pulses. The non-linear phase refocusing pulses has been designed to operate at a lower maximum B1 requirement (0.15 G) while keeping the pulse width short (4.3 ms) and maintaining adequate bandwidth for spectroscopy application at 3T (1.2 kHz). At a TE of 42 ms, the short inter pulse delay (10.5 ms) between the refocusing pulses has a potential to provide improved sensitivity for J-coupled metabolites such as myoinositol (mI) and glutamate / glutamine (Glx) over conventional short TE (35 ms) PRESS sequence.

I. Hancu, Which pulse sequence is optimal for myo-inositol detection at 3T? NMR Biomed, 22: 426 – 435 (2009) https://doi.org/10.1002/nbm.1353

I. Hancu et al, Improved Myo-inositol Detection Through Carr–Purcell PRESS: A Tool for More Sensitive Mild Cognitive Impairment Diagnosis, Magn Reson Med, 65: 1515 – 1521 (2011) https://doi.org/10.1002/mrm.22749


JPRESS

The two-dimensional J-resolved spectroscopy sequence consists of a series of spin-echo experiments with different echo times defined by the average echo time (TE) and the delta of echo times (User CV 16) employing PRESS localization. Adding the spectra gives a TEA-PRESS spectrum.

L. Ryner et al., Localized 2D J-resolved H-1 MR spectroscopy – strong coupling effects in vitro and in vivo, Magn Reson Imaging, 13: 853 – 869 (1995) https://doi.org/10.1016/0730-725x(95)00031-b

R. Schulte, Improved two-dimensional J-resolved spectroscopy, NMR Biomed, 19: 264 – 270 (2006) https://doi.org/10.1002/nbm.1027


mBREASE

mBREASE is a TEA-PRESS sequence with enabled STIR fat suppression, storage of each aquired FID to correct for frequency shifts and acquisition of reference data with different echo times to correct for water T2. It includes quantification of the choline signal using a voigt-lineshape model function in time domain and linear baseline in frequency domain. T2 corrected water signal is used as internal reference.


Editing

Spectral j-difference editing describes an advanced spectroscopy acquisition technique which is generally necessary to detect j-coupled markers and separate from co-resonant metabolite peaks. The implemented editing technique is based on the BASING technique described.

J. Star-Lack et al., Improved Water and Lipid Suppression for 3D PRESS CSI Using RF Band Selective Inversion with Gradient Dephasing (BASING), Magn Reson Med, 38, 311 – 321, (1997) https://doi.org/10.1002/mrm.1910380222

J. Star-Lack et al., In Vivo Lactate Editing with Simultaneous Detection of Choline, Creatine, NAA, and Lipid Singlets at 1.5 T Using PRESS Excitation with Applications to the Study of Brain and Head and Neck Tumors, J Magn Reson, 133: 243 – 254 (1998) https://doi.org/10.1006/jmre.1998.1458


BS-PRESS

BS-PRESS is a voxel based TG calibration method described in [8]. The phase-based B1+ mapping technique using the Bloch-Siegert shift method encodes the B1 information into a signal phase resulting from off-resonant RF pulses within the sequence [9-11].

8. R. Noeske et al., Voxel Based Transmit Gain Calibration using Bloch-Siegert Shift Method for MR Spectroscopy, Proc 20th Annual Meeting ISMRM, Melbourne: 1733 (2012)

9. Sacolick et al., B1 Mapping by Bloch-Siegert Shift, Magn Reson Med, 63: 1315 - 1322 (2010)

10. Sacolick et al., Fast Radiofrequency Flip Angle Calibration by Bloch–Siegert Shift, Magn Reson Med, 66: 1333 - 1338 (2011)

11. Sacolick et al., Fast Spin Echo Bloch-Siegert B1 Mapping, Proc 19th Annual Meeting ISMRM, Montreal: 2927 (2011)



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