Method and apparatus for rapid spin echo magnetic resonance imaging

Claim 2

Method for magnetic resonance imaging of a body placed in a stationary and substantially homogeneous main magnetic field, the method comprising repeated execution, with a repetition time TR, of a sequence including the following steps: application of a first RF-pulse for excitation of at least a portion of the body, application of at least a first gradient magnetic field for phase encoding of the excited portion, application of a second RF-pulse at a time τ after the first RF-pulse, detection of a magnetic resonance spin-echo signal around a time 2τ after the first RF-pulse, wherein: the repetition time TR between the first RF-pulses in subsequent sequences is shorter than a transverse relaxation time T 2 of a relevant substance of the body, said first gradient magnetic field is applied after the application of the second RF-pulse, and a second gradient magnetic field for compensation of the phase encoding caused by the first gradient magnetic field is applied in the interval after occurrence of the magnetic resonance spin-echo signal and before application of the first RF-pulse in a next sequence.

Claim 3

Method as claimed in claim 1, characterised in that a selection gradient magnetic field is applied during application of the first RF-pulse for selection of a slice of the body, and in that a third gradient magnetic field is applied during detection of the magnetic resonance spin-echo signal for frequency encoding.

Claim 4

Method as claimed in claim 1 characterised in that phase differences between the first RF-pulse and the second RF-pulses within a sequence are equal over the sequences.

Claim 5

Method as claimed in claim 3, characterised in that the first RF-pulses in subsequent sequences have zero phase difference and in that the second RF-pulses in subsequent sequences have zero phase difference.

Claim 6

Method as claimed in claim 3, characterised in that the phases of the first and second RF-pulses in subsequent sequences are mutually different, thereby forming an RF-spoiling scheme.

Claim 7

Method as claimed in claim 5, characterised in that the phases of the first and second RF-pulses are changed from one sequence to another according to a non-repetitive scheme.

Claim 8

Method as claimed in claim 6, characterised in that the phases of the first and second RF-pulses in successive sequences differ with a linear increasing or decreasing value proportional to a rank number of the sequence.

Claim 9

Method as claimed in claim 1, characterised in that the repetition time TR is about 50 milliseconds or less.

Claim 10

Apparatus for magnetic resonance imaging comprising means for establishing a stationary and substantially homogeneous main magnetic field, means for generating gradient magnetic field superimposed upon the main magnetic field, means for radiating RF-pulses towards a body placed in the main magnetic field, control means for controlling the generation of the gradient magnetic fields and the RF-pulses, and means for receiving and sampling magnetic resonance signals generated by sequences of RF-pulses and switched gradient magnetic fields, said control means being meant for: applying a first radio-frequency pulse for excitation of at least a portion of the body, applying at least a first gradient magnetic field for phase encoding of the excited portion, applying a second RF-pulse at a time τ after the first RF-pulse, and detecting a magnetic resonance spin-echo signal around a time 2τ after the first RF-pulse, in a sequence which is repeatedly executed with a repetition time TR between first RF-pulses in subsequent sequences that is shorter than a transverse relaxation time T 2 of a relevant substance of the body, characterised in that the control means are further arranged for applying said first gradient magnetic field after the application of the second RF-pulse, and applying a second gradient magnetic field in the interval after occurrence of the magnetic resonance spin-echo signal and before application of the first RF-pulse in a next sequence, the second gradient magnetic field compensating the phase encoding caused by the first gradient magnetic field.

Claim 11

Apparatus for magnetic resonance imaging comprising means for establishing a stationary and substantially homogeneous main magnetic field, means for generating gradient magnetic field superimposed upon the main magnetic field, means for radiating RF-pulses towards a body placed in the main magnetic field, control means for controlling the generation of the gradient magnetic fields and the RF-pulses, and means for receiving and sampling magnetic resonance signals generated by sequences of RF-pulses and switched gradient magnetic fields, said control means being meant for: applying a first radio-frequency pulse for excitation of at least a portion of the body, applying at least a first gradient magnetic field for phase encoding of the excited portion, applying a second RF-pulse at a time τ after the first RF-pulse, and detecting a magnetic resonance spin-echo signal around a time 2τ after the first RF-pulse, in a sequence which is repeatedly executed with a repetition time TR between first RF-pulses in subsequent sequences that is shorter than a transverse relaxation time T 2 of a relevant substance of the body, characterised in that the control means are further arranged for applying said first gradient magnetic field after the application of the second RF-pulse, and applying a second gradient magnetic field in the interval after occurrence of the magnetic resonance spin-echo signal and before application of the first RF-pulse in a next sequence, the second gradient magnetic field compensating the phase encoding caused by the first gradient magnetic field.

Claim 12

Method as claimed in claim 2, characterized in that phase differences between the first RF-pulse and the second RF-pulses within a sequence are equal over the sequences.

Claim 13

Method as claimed in claim 10, characterized in that the first RF-pulses in subsequent sequences have zero phase difference and in that the second RF-pulses in subsequent sequences have zero phase difference.

Claim 14

Method as claimed in claim 10, characterized in that the phases of the first and second RF-pulses in subsequent sequences are mutually different, thereby forming an RF-spoiling scheme.

Claim 15

Method as claimed in claim 12, characterized in that the phases of the first and second RF-pulses are changed from one sequence to another according to a non-repetitive scheme.

Claim 16

Method as claimed in claim 13, characterized in that the phases of the first and second RF-pulses in successive sequences differ with a linear increasing or decreasing value proportional to a rank number of the sequence.

Claim 17

Method as claimed in claim 2, characterised in that the repetition time TR is about 50 milliseconds or less.

Claim 18

Method as claimed in claim 3, characterised in that the repetition time TR is about 50 milliseconds or less.

Claim 19

Method as claimed in claim 4, characterised in that the repetition time TR is about 50 milliseconds or less.

Claim 20

Method as claimed in claim 11, characterised in that the repetition time TR is about 50 milliseconds or less.

Claim 21

Method as claimed in claim 12, characterised in that the repetition time TR is about 50 milliseconds or less.

Claim 22

Method as claimed in claim 1 wherein said first RF-pulse has a flip-angle substantially greater than 90° and less than 180° and said second RF-pulse has a flip-angle substantially equal to 180°.