Method and control device to operate a magnetic resonance system

• US 9,476,955 B2
• Filed: 03/20/2013
• Issued: 10/25/2016
• Est. Priority Date: 03/20/2012
• Status: Active Grant

• Current Assignee: Siemens Healthineers AG (Siemens AG)
• Original Assignee: Siemens AG
• Inventors: Stemmer, Alto
• Primary Examiner(s): Vargas, Dixomara
• Application Number:
  US13/847,656
• Publication Number:
  US 20130249548A1
• Time in Patent Office: 1,315 Days
• US Class Current: 1/1
• CPC Class Codes: A61B 5/055 involving electronic [EMR] or nuclear [NMR] magnetic resonance, e.g. magnetic resonance imaging
• CPC Class Codes: G01R 33/44 using nuclear magnetic resonance [NMR] G01R33/24, G01R33/62 take precedence
• CPC Class Codes: G01R 33/4824 using a non-Cartesian trajectory
• CPC Class Codes: G01R 33/4835 of multiple slices
• CPC Class Codes: G01R 33/543 Control of the operation of the MR system, e.g. setting of acquisition parameters prior to or during MR data acquisition, dynamic shimming, use of one or more scout images for scan plane prescription G01R33/546 takes precedence

Abstract

In a method and a control device for operation of a magnetic resonance tomography system to generate image data, multiple of slices in an examination subject are initially excited at a first time interval by a respective RF slice excitation pulse of a series of spatially selective slice excitation pulses. An RF refocusing pulse is then emitted at a second time interval after the first excitation pulse or after the last excitation pulse of the series of RF slice excitation pulses. At least one additional RF refocusing pulse is emitted at a third time interval after a preceding RF refocusing pulse. The third time interval is twice as long as the second time interval. The width of the RF refocusing pulses is selected to generate a number of chronologically separate echo signals per RF refocusing pulse for simultaneous refocusing of all excited slices.

Claims

1. A method to operate a magnetic resonance tomography system having a magnetic resonance data acquisition scanner that has a radio-frequency (RF) radiator and a gradient coil arrangement comprising:

operating the RF radiator to excite nuclear spins in a plurality of slices in an examination subject in said magnetic resonance data acquisition scanner at a first time interval by radiating a series of spatially selective RF slice excitation pulses, with each RF slice excitation pulse in said series exciting nuclear spins in a respective slice in said plurality of slices;

operating the RF radiator to emit an RF refocusing pulse in said magnetic resonance data acquisition scanner at a second time interval after a first RF excitation pulse or after a last RF excitation pulse in said series of spatially selective RF slice excitation pulses, and emitting at least one additional RF refocusing pulse at a third time interval after a preceding RF refocusing pulse, with said third interval to being twice as long as said second time interval, and with each of said RF refocusing pulses having a width so as to generate a plurality of chronologically successive separate echo signals for each RF refocusing pulse, with each RF refocusing pulse being simultaneously effective in multiple excited slices among said plurality of slices;

operating the gradient coil arrangement to read out said echo signals for each refocusing pulse under a readout gradient in a corresponding number of readout windows; and

providing the echo signals that have been read out to a processor and in said processor, converting said echo signals into magnetic resonance data and making said magnetic resonance data available from said processor in electronic form, as a data file.

2. A method as claimed in claim 1 comprising operating said gradient coil arrangement to activate said gradient pulse series between two successive RF slice excitation pulses that have a 0th moment equal to an accumulated 0th moment of said gradient pulse series.

3. A method as claimed in claim 2 comprising operating said gradient coil arrangement to activate said gradient pulse series with the 0th moment of all gradient pulses activated in the slice selection direction between isodelay points of two successive RF excitation pulses being zero.

4. A method as claimed in claim 2 comprising operating said gradient coil arrangement to activate said gradient pulse series with a 0th moment accumulated as a result of an activated gradient pulse in said readout direction between said last RF excitation pulse and a first RF refocusing pulse in said series of RF refocusing pulses being equal to the 0th moment accumulated in the readout direction between said first of said RF refocusing pulses and a first of said echo signals.

5. A method as claimed in claim 1 comprising operating said RF radiator with a time duration of each RF slice excitation pulse being shorter than a time duration of any RF refocusing pulse.

6. A method as claimed in claim 5 comprising operating said gradient coil arrangement to activate said gradient pulse series to scan respective k-spaces of the respective slices in a single echo train either once or twice.

7. A method as claimed in claim 5 comprising operating said magnetic resonance data acquisition scanner with a pulse sequence comprised of multiple sequence modules, each having an echo train, and acquiring raw data of at least two segments of k-space for each slice with each echo train.

8. A method as claimed in claim 7 comprising operating said magnetic resonance data acquisition scanner to segment the respective k-spaces according to a PROPELLER trajectory.

9. A method as claimed in claim 7 comprising operating said magnetic resonance data acquisition scanner to acquire said magnetic resonance data from different segments of a respective slice in different sequence modules, with a timing of the respective RF slice excitation pulse for the respective slice being varied from pulse sequence-to-pulse sequence.

10. A method as claimed in claim 5 comprising:

operating said RF radiator to excite said plurality of slices in a magnetic resonance pulse sequence module comprising a plurality of readout windows and operating said gradient coil arrangement to acquire the data from the respective slices in respectively different ones of said readout windows individually associated with respective RF refocusing pulses;

in said processor, calculating separate magnitude images from the magnetic resonance data acquired from the plurality of readout windows; and

in said processor, combining said magnitude images associated with a same slice into a single slice image of said same slice, and making said single slice image available from said processor in electronic form as am image data file.

11. A method as claimed in claim 10 comprising combining said magnitude images in said processor using a sum-of-squares technique.

12. A method as claimed in claim 5 comprising:

operating said RF radiator to excite said plurality of slices in a magnetic resonance pulse sequence module comprising a plurality of readout windows and operating the gradient coil arrangement to acquire the data from the respective slices in respectively different ones of said readout windows individually associated with respective RF refocusing pulses; and

in said processor, calculating image data from said magnetic resonance data and combining image data of a respective slice that were acquired with a single echo train in different ones of said readout windows in a complex-value combination of said image data.

13. A method as claimed in claim 12 comprising combining said image data after computationally removing a phase associated with the image data.

14. A control device to operate a magnetic resonance tomography system comprising:

a computerized control unit comprising an interface configured to place said control unit in communication with a magnetic resonance data acquisition scanner to provide control signals to said magnetic resonance data acquisition scanner to excite nuclear spins in a plurality of slices in an examination subject in said magnetic resonance data acquisition scanner at a first time interval by radiating a series of spatially selective RF slice excitation pulses, with each RF slice excitation pulse in said series exciting nuclear spins in a respective slice in said plurality of slices;

said control unit being configured to cause said data acquisition unit to emit an RF refocusing pulse in said data acquisition scanner at a second time interval after a first RF excitation pulse or after a last RF excitation pulse in said series of spatially selective RF excitation pulses, and to emit at least one additional RF refocusing pulse at a third time interval after a preceding RF refocusing pulse; and

said control unit being configured to set said third time interval to be twice as long as said second time interval, and to set a width of each of said RF refocusing pulses so as to generate a plurality of chronologically successive separate echo signals for each RF refocusing pulse, with each RF refocusing pulse being simultaneously effective in multiple excited slices among said plurality of slices.

15. A magnetic resonance tomography apparatus comprising:

a magnetic resonance data acquisition scanner;

a control computer configured to operate said data acquisition scanner to excite nuclear spins in a plurality of slices in an examination subject in said magnetic resonance data acquisition scanner at a first time interval by radiating a series of spatially selective RF slice excitation pulses, with each RF slice excitation pulse in said series exciting nuclear spins in a respective slice in said plurality of slices;

said control computer being configured to operate said data acquisition scanner to emit an RF refocusing pulse in said data acquisition unit at a second time interval after a first RF excitation pulse or after a last RF excitation pulse in said series of spatially selective RF excitation pulses, and to emit at least one additional RF refocusing pulse at a third time interval after a preceding RF refocusing pulse; and

said control computer being configured to set said third time interval to be twice as long as said second time interval, and to set a width of each of said RF refocusing pulses so as to generate a plurality of chronologically successive separate echo signals for each RF refocusing pulse, with each RF refocusing pulse being simultaneously effective in multiple excited slices among said plurality of slices.

16. A non-transitory, computer-readable data storage medium encoded with programming instructions, said storage medium being loaded into a computerized control and evaluation computer system of a magnetic resonance tomography system that also comprises a magnetic resonance data acquisition scanner, said programming instructions causing said control and evaluation computer system to:

operate said data acquisition scanner to excite nuclear spins in a plurality of slices in an examination subject in said magnetic resonance data acquisition scanner at a first time interval by radiating a series of spatially selective RF slice excitation pulses, with each RF slice excitation pulse in said series exciting nuclear spins in a respective slice in said plurality of slices;

operate said data acquisition scanner to emit an RF refocusing pulse in said data acquisition unit at a second time interval after a first RF excitation pulse or after a last RF excitation pulse in said series of spatially selective RF excitation pulses, and to emit at least one additional RF refocusing pulse at a third time interval after a preceding RF refocusing pulse; and

set said third time interval to be twice as long as said second time interval, and set a width of each of said RF refocusing pulses so as to generate a plurality of chronologically successive separate echo signals for each RF refocusing pulse, with each RF refocusing pulse being simultaneously effective in multiple excited slices among said plurality of slices.