IR/SR TrueFISP. Works-in-Progress package Version 1.2. For the SIEMENS Magnetom. Installation and User s Guide NUMARIS/4VA21B.

Similar documents
Works-in-Progress package Version 1.0. For the SIEMENS Magnetom. Installation and User s Guide NUMARIS/4VA21B. January 22, 2003

Cardiac MR. Dr John Ridgway. Leeds Teaching Hospitals NHS Trust, UK

Pulse Sequence Design and Image Procedures

(N)MR Imaging. Lab Course Script. FMP PhD Autumn School. Location: C81, MRI Lab B0.03 (basement) Instructor: Leif Schröder. Date: November 3rd, 2010

Background (~EE369B)

Application Guide & Release Notes

Pulse Sequence Design Made Easier

Principles of MRI EE225E / BIO265. Lecture 21. Instructor: Miki Lustig UC Berkeley, EECS. M. Lustig, EECS UC Berkeley

Steady-state sequences: Spoiled and balanced methods

Gradient Spoiling. Average balanced SSFP magnetization Reduce sensitivity to off-resonance. FFE, FISP, GRASS, GRE, FAST, Field Echo

HETERONUCLEAR IMAGING. Topics to be Discussed:

Lab 8 6.S02 Spring 2013 MRI Projection Imaging

MRI Summer Course Lab 2: Gradient Echo T1 & T2* Curves

Module 2. Artefacts and Imaging Optimisation for single shot methods. Content: Introduction. Phase error. Phase bandwidth. Chemical shift review

H Micro-Imaging. Tuning and Matching. i. Open any 1H data set and type wobb.

BOLD fmri: signal source, data acquisition, and interpretation

6.S02 MRI Lab Acquire MR signals. 2.1 Free Induction decay (FID)

Pulse Sequences: Rapid Gradient Echo

2015 Spin echoes and projection imaging

MR Advance Techniques. Flow Phenomena. Class II

H 2 O and fat imaging

1 Introduction. 2 The basic principles of NMR

Experience in implementing continuous arterial spin labeling on a commercial MR scanner

functional MRI: A primer

Diff Ganzkörper ep2d_diff_stir_b50_800_tra

High Field MRI: Technology, Applications, Safety, and Limitations

RAD 229: MRI Signals and Sequences

Advanced MSK MRI Protocols at 3.0T. Garry E. Gold, M.D. Associate Professor Department of Radiology Stanford University

NIH Public Access Author Manuscript Magn Reson Med. Author manuscript; available in PMC 2010 July 21.

Variable-Rate Selective Excitation for Rapid MRI Sequences

MR Basics: Module 8 Image Quality

Clear delineation of optic radiation and very small vessels using phase difference enhanced imaging (PADRE)

Applications Guide. Spectral Editing with SVS. (Works-in-Progress) MAGNETOM TaTs and Verio Systems (3T)

Simultaneous Multi-Slice (Slice Accelerated) Diffusion EPI

Slice profile optimization in arterial spin labeling using presaturation and optimized RF pulses

Improve Image Quality of Transversal Relaxation Time PROPELLER and FLAIR on Magnetic Resonance Imaging

MR Basics: Module 6 Pulse Sequences

MRI Metal Artifact Reduction

Page 1 of 9. Protocol: adult_other_adni3_study_human_ge_3t_25w_ _ _1. 3 Plane Localizer. 3 Plane Localizer PATIENT POSITION

Gradients. Effects of B0 gradients on transverse magnetisation Similar to figure 10 of Sattler review Progr. NMR 34 (1999), 93

COMMUNICATIONS Volume-Selective Multipulse Spin-Echo Spectroscopy

Lesson 06: Pulse-echo Imaging and Display Modes. These lessons contain 26 slides plus 15 multiple-choice questions.

2014 M.S. Cohen all rights reserved

MRI imaging in neuroscience Dr. Thom Oostendorp Lab class: 2 hrs

Localization of microscale devices in vivo using addressable transmitters operated as magnetic spins

Inherent Insensitivity to RF Inhomogeneity in FLASH Imaging

Mapping the Flip Angle in Magnetic Resonance Imaging Using the Accelerated 3D Look-Locker Sequence

k y 2k y,max k x 2k x,max

Magnetic Resonance Imaging Principles, Methods, and Techniques

EE469B: Assignment 2 Solutions

SIEMENS MAGNETOM Skyra syngo MR D13

Quick Reference Guide

PHYS225 Lecture 18. Electronic Circuits

EPISTAR MRI: Multislice Mapping of Cerebral Blood Flow

Magnetic Resonance Imaging

NIH Public Access Author Manuscript Magn Reson Med. Author manuscript; available in PMC 2009 December 1.

The SENSE Ghost: Field-of-View Restrictions for SENSE Imaging

Arrayed Acquisition in VNMR and on the Gemini 1

10. Phase Cycling and Pulsed Field Gradients Introduction to Phase Cycling - Quadrature images

PHY3902 PHY3904. Nuclear magnetic resonance Laboratory Protocol

Noninvasive Blood Flow Mapping with Arterial Spin Labeling (ASL) Paul Kyu Han and Sung-Hong Park

Half-Pulse Excitation Pulse Design and the Artifact Evaluation

In a typical biological sample the concentration of the solute is 1 mm or less. In many situations,

Spiral MRI on a 9.4T Vertical-bore Superconducting Magnet Using Unshielded and Self-shielded Gradient Coils

DT 9818 Waveform-Generator. Hardware Trigger Version. Operating Manual. Version 2.0. May Page 1 of 21

LSM 780 Confocal Microscope Standard Operation Protocol

Steady-state MRI: methods for neuroimaging

Supplementary Figure 1. Scanning Electron Microscopy images of the pristine electrodes. (a) negative electrode and (b) positive electrode.

SpinCore RadioProcessor LabVIEW Extensions

Field Simulation Software to Improve Magnetic Resonance Imaging

Physics Experiment N -17. Lifetime of Cosmic Ray Muons with On-Line Data Acquisition on a Computer

1D Transient NOE on the Bruker DRX-500 and DRX-600

A. SPECIFIC AIMS: phase graph (EPG) algorithms to cover a wide range of MRI

ScanArray Overview. Principle of Operation. Instrument Components

Encoding of inductively measured k-space trajectories in MR raw data

Confocal imaging on the Leica TCS SP8. 1) Turn the system on. 2) Use TCS user account. 3) Start LAS X software:

SPECT Reconstruction & Filtering

LSM 710 Confocal Microscope Standard Operation Protocol

Fundamental and Clinical Studies for Effectiveness of Zero-filling Interpolation on k-space for Improvement of Sharpness in Magnetic Resonance Imaging

ACRIN 6686 / RTOG 0825

Optimizing the Magnetization-Prepared Rapid Gradient-Echo (MP-RAGE) Sequence

Nikon A1R. Multi-Photon & Laser Scanning Confocal Microscope. Kyle Marchuk Adam Fries Jordan Briscoe Kaitlin Corbin. April 2017.

The promise of high-field MRI. High Field MRI Technology, Applications, Safety, and Limitations. High-field Scanners

Image Quality/Artifacts Frequency (MHz)

RF Pulse Toolkit: Application Specific Design

Radio Frequency Field

Training Guide for Leica SP8 Confocal/Multiphoton Microscope

Confocal Application Notes Vol. 5 July 2010

Tissue classification based on relaxation environments

2D, 3D CT Intervention, and CT Fluoroscopy

EE225E/BIOE265 Spring 2014 Principles of MRI. Assignment 6. Due Friday March 7th, 2014, Self Grading Due Monday March 10th, 2014

Gradient hysteresis in MRI and NMR experiments

3T Unlimited. ipat on MAGNETOM Allegra The Importance of ipat at 3T. medical

Apple Photos Quick Start Guide

MRI Anatomy and Positioning Series Module 12: Fat Suppression Techniques

Improving high-field MRI using parallel excitation

Brief Operation Manual for Imaging on BX61W1

Your first NMR measurement

Supplementary Discussion 1: NV center level diagram

SmartExam helps to banish most repeat knee studies at Desert Medical Imaging

Transcription:

Works-in-Progress package Version 1.2 For the Installation and User s Guide NUMARIS/4VA21B January 22, 2003 Section of Medical Physics, University Hospital Freiburg, Germany Contact: Klaus Scheffler PhD + Simone Peschl PhD, Hugstetterstr. 55, D 79106 Freiburg, email: Klaus.scheffler@unibas.ch

Table of Contents 1 Basic principles... 3 1.1 Sequence structure and timing... 3 1.2 References... 4 2 Software Installation Procedure... 5 2.1 Installation... 5 2.2 Restart the System... 5 3 Sequences and Protocols... 6 3.1 Single slice mode... 6 3.2 Multi slice mode... 8 3.3 Calculation of T1 and M0 map... 9 3.4 Tips and tricks... 10 Page 2 of 10

1 Basic principles The basic principle of T1 quantification with inversion prepared TrueFISP can be found in reference (1,2). After an inversion pulse acquisition is started with a TrueFISP sequence that detects the relaxing magnetization. The influence of the TrueFISP excitation pulse train on the recovering magnetization is relatively small compared to T1-weighted FLASH, as can be seen in the figure: 10000 TrueFISP 10 TrueFISP 50 FLASH 5 5000 reference FLASH 10 echo amplitude (a.u.) 0-5000 FLASH 20 TR = 3 ms for FLASH/TrueFISP NiSO 4 phantom (T 1 =260 ms) -10000 0 200 400 600 800 time after inversion pulse in ms Therefore, an exponential fit to the measured relaxation curve gives a reasonable estimation of the T1 relaxation time and proton density M0. 1.1 Sequence structure and timing Imaging is performed with a conventional, ramped α-prepared 2D TrueFISP sequence. RF and echo spacing is equal to 2TE. For single slice imaging the positioning of the inversion/saturation slab and imaging slice is independent and free. For multi slice imaging the inversion/saturation slab is always parallel to the imaging slices. In this case the thickness of the inversion/saturation slab is 1.5 times the thickness if the imaging slices. Therefore a slice distance of at least 70% should be selected. Selective inversion pulses are based on an optimized adiabatic full passage pulse, and selective saturation pulses on an optimized SLR pulse (included in external file hypersec.pls). After inversion/saturation an α/2 prepared TrueFISP train starts that acquires several identical segments of Page 3 of 10

the k-space. After TR the next acquisition of a second segment is started. The number of different segments required to fill the k-space gives the number of repetitions that have to be acquired. The number of identical segments within one TR gives the number of images with different inversion times TI. The timing and k-space acquisition scheme is thus identical the segmented cine imaging used in cardiac applications. inversion/saturation segmented TrueFISP imaging segment TI1 TI2 TI3 TR TIn 1.2 References (1) Deimling M, Heid O. Magnetization prepared true FISP imaging. In: Proceedings of the Second Annual Meeting of the Society of Magnetic Resonance, San Francisco 1994 ;p. 495. (2) Scheffler K, Hennig J. T1 quantification with inversion recovery TrueFISP. Magnet Reson Med 2001; 45(4): 720-723. Page 4 of 10

2 Software Installation Procedure Note: This package can only be used in combination with an IDEA licence! 2.1 Installation The IR TrueFISP installation CD contains the following files: 1. The Word document WIP-IRT1_trufi_VA21B.doc 2. A folder named protocol that contains 2.1. A file named WIP.edx 2.2. A folder named WIP.edxdir To install the WIP package please: 1. Place the CD in the drive tray. 2. Open the Exam Explorer. 3. Open a program region and a subprogram region. 4. Click on this subprogram region and select Object/Import. 5. Select the CD drive in the pop-up window, double-click on the folder protocol and select the file WIP.edx. To install the external RF pulse and image reconstruction ICE program please: 6. Place the CD in the drive tray. 7. Open the Windows NT Explorer (with control-escape). 8. Select the CD drive 9. Go to folder protocol/wip.edxdir/customerseq. 10. Copy the file hypersec.pls to C/MedCom/MriSiteData/measurement/. 11. Change to drive Q (MedCom on 192.168.2.3 (Q:)) and create the directory Q/MriCustomer/IcePrograms. 12. Select the CD drive 13. Go to folder protocol/wip.edxdir/customerseq. 14. Copy the file IceProgramT1TrueFisp.dll to Q/MriCustomer/IcePrograms/. 15. Close the Windows NT Explorer and eject CD. 2.2 Restart the System In order for the changes to take effect (external RF pulse), you will need to restart System. Page 5 of 10

3 Sequences and Protocols 3.1 Single slice mode The positioning of the slice and the inversion/saturation slab is free and independent. The inversion/saturation slab can be accessed and modified via the UI on the Geometry/Saturation card: The selection between inversion and saturation can be done in the Contrast card: Page 6 of 10

The number n of images with different inversion times TI(1) TI(n) can be selected via the number of contrasts given in the Sequence/Part1 card. The corresponding inversion times depend on the segmentation of the k-space. If partial k-space is selected (7/8 or 6/8) the time interval between consecutive inversion times is not equidistant. The number of segments can be chosen in the Sequence/Part2 card: Page 7 of 10

The reordering of the segments into k-space can be sequential or interleaved, which can be selected in the Sequence/Special card. Interleaved reordering is recommended. 3.2 Multi slice mode In the multi slice mode the position of the inversion/saturation slabs is automatically parallel to the imaging slices. The thickness of the inversion/saturation slabs is roughly 1.5 times that of the imaging slices. Therefore the slice distance should be at least about 70%. The display of these slabs is switched off and only the position of the imaging slices is visible. As in multi slice spin echo imaging the TR corresponds to the repetition time of the inversion/saturation pulses within the same slice. Further parameters are identical to the single slice mode. Note: if you go back to single slice mode you have to reactivate the free inversion/saturation slab on the Geometry/Saturation card by clicking the + button. Page 8 of 10

3.3 Calculation of T1 and M0 map The number of calculated images is equal to the number of slices times the number of contrasts (different inversion times). If the check box T1 map is activated on the Sequence/Special card the reconstruction program will additionally calculate a T1 and M0 map. This feature can be used both for inversion or saturation recovery. The gray values of the T1 map corresponds to the T1 value in ms. The gray values of the M0 map is proportional to the proton density. Page 9 of 10

3.4 Tips and tricks The number of contrasts (i.e. different inversion/saturation times) and the time interval between successive inversion/saturation times (controlled by the number of segments) should be chosen carefully in order to provide an efficient sampling of the relaxation curve. Too long or too short inversion/saturation times will give poor T1 and M0 estimations. A short TR will decrease the M0 value. There is also some systematic error in the T1 estimation due to saturation effects of the TrueFISP sequence. The flip angle should therefore be less or equal 40. If the T1/M0 fitting routine is not able to calculate reasonable values (i.e. less than 3 inversion/saturation times, signal too small, no zero crossing of the inversion curve) T1 and M0 is set to zero. Page 10 of 10