Magnetic resonance imaging method

Claim 1

A method of NMR or ESR, or the like imaging in which an RF magnetic field pulse, a slice magnetic field, a phase encoding magnetic field and a signal reading magnetic field are applied to a sample in a predetermined sequence, for the construction of a desired slice image on the basis of a magnetic resonance signal from the sample, comprising the steps of: applying a first signal reading magnetic field having a predetermined pulse area; applying a second signal reading magnetic field having a pulse area twice that of said predetermined pulse area and having a polarity opposite to that of said first signal reading magnetic field; and applying a third signal reading magnetic field having the same polarity as that of said first signal reading magnetic field, said steps of applying said first signal reading magnetic field, applying said second signal reading magnetic field and applying said third signal reading magnetic field are performed in the interval from the application of the RF magnetic field pulse and until a magnetic resonance signal is obtained, and the peak value of said magnetic resonance signal is obtained when the pulse area of said third signal reading magnetic field becomes equal to said predetermined pulse area.

Claim 2

A method of NMR or ESR, or the like imaging in which an RF magnetic field pulse, a slice magnetic field, a phase encoding magnetic field and a signal reading magnetic field are applied to a sample in a predetermined sequence, for the construction of a desired slice image on the basis of a magnetic resonance signal from the sample, comprising the steps of: applying a first signal reading magnetic field having a predetermined pulse area; applying a second signal reading magnetic field having a pulse area twice that of said predetermined pulse area and having a polarity opposite to that of said first signal reading magnetic field; and applying a third signal reading magnetic field having the same polarity as that of said first signal reading magnetic field, said steps of applying said first signal reading magnetic field, applying said second signal reading magnetic field and applying said third signal reading magnetic field are performed in the interval from the application of the RF magnetic field pulse and until a magnetic resonance signal is obtained, and the peak value of said magnetic resonance signal is obtained when the pulse area of said third signal reading magnetic field becomes equal to said predetermined pulse area.

Claim 3

A method of magnetic resonance imaging for constructing a desired slice image of a sample in an imaging region on the basis of magnetic resonance signals, said method comprising the steps of: repeating a sequence comprising applying an RF magnetic field pulse, a slice magnetic field, a phase encoding magnetic field and a signal reading magnetic field, and collecting the magnetic resonance signals from the sample; varying phase encoding coefficients in accordance with body movement of the sample, said phase encoding coefficients determining phase encoding amounts; and applying said determined phase encoding amounts to the imaging region in a field of view of the sample, whereby the relative position of the imaging region is maintained.

Claim 4

A method of magnetic resonance imaging for constructing a desired slice image of a sample in an imaging region on the basis of magnetic resonance signals, said method comprising the steps of: repeating a sequence comprising applying an RF magnetic field pulse, a slice magnetic field, a phase encoding magnetic field and a signal reading magnetic field, and collecting the magnetic resonance signals from the sample; varying phase encoding coefficients in accordance with body movement of the sample, said phase encoding coefficients determining phase encoding amounts; and applying said determined phase encoding amounts to the imaging region in a field of view of the sample, whereby the relative position of the imaging region is maintained.

Claim 5

A method of magnetic resonance imaging comprising the steps of: repeating a sequence including applying an RF pulse, a slice magnetic field, a signal reading magnetic field and a phase encoding magnetic field to a sample, and collecting MR signals from the sample; varying a phase encoding amount Ki due to said phase encoding magnetic field responsive to the order of signal collection i; and constructing a slice image from said MR signals that have been collected, wherein at least one of a slice magnetic field Gs(t) applied in accordance with said RF pulse, a signal reading magnetic field GR(t) applied in accordance with said MR signal, and a phase encoding magnetic field Ge(t) is divided into a plurality of pulses, and the areas of the pulses with the polarity being considered are set as to satisfy, (a) with respect to said slice magnetic field Gs(t), the relationship on the integral from a central position of said RF pulse, ∫r Gs(t) Ps(t) dt=0, (b) with respect to said signal reading magnetic field Gr(t), the relationship on the integral to a central position of said MR signals, ∫r Gr(t) Pr(t) dt=0, and (c) with respect to the phase encoding magnetic field Ge(t), the relationship on the integral ∫r Ge(t) Pe(t) dt=Ki, where r represents a gyromagnetic ratio, and Ps(t), Pr(t) and Pe(t) represent components of the position of an object nucleus in the directions of the respective gradient magnetic fields.

Claim 6

A method of magnetic resonance imaging comprising the steps of: repeating a sequence including applying an RF pulse, a slice magnetic field, a signal reading magnetic field and a phase encoding magnetic field to a sample, and collecting MR signals from the sample; varying a phase encoding amount Ki due to said phase encoding magnetic field responsive to the order of signal collection i; and constructing a slice image from said MR signals that have been collected, wherein at least one of a slice magnetic field Gs(t) applied in accordance with said RF pulse, a signal reading magnetic field GR(t) applied in accordance with said MR signal, and a phase encoding magnetic field Ge(t) is divided into a plurality of pulses, and the areas of the pulses with the polarity being considered are set as to satisfy, (a) with respect to said slice magnetic field Gs(t), the relationship on the integral from a central position of said RF pulse, ∫r Gs(t) Ps(t) dt=0, (b) with respect to said signal reading magnetic field Gr(t), the relationship on the integral to a central position of said MR signals, ∫r Gr(t) Pr(t) dt=0, and (c) with respect to the phase encoding magnetic field Ge(t), the relationship on the integral ∫r Ge(t) Pe(t) dt=Ki, where r represents a gyromagnetic ratio, and Ps(t), Pr(t) and Pe(t) represent components of the position of an object nucleus in the directions of the respective gradient magnetic fields.

Claim 7

A method of magnetic resonance imaging in which magnetic resonance is utilized, comprising imaging the time derivative of the position of object spins which move.

Claim 8

A method of magnetic resonance imaging in which magnetic resonance is utilized, comprising imaging the time derivative of the position of object spins which move.

Claim 15

A method of magnetic resonance imaging comprising imaging a product of a time derivative of the position of object spins which move and spin density.

Claim 16

A method of magnetic resonance imaging comprising imaging a product of a time derivative of the position of object spins which move and spin density.