Method for suppression of acoustic ringing in NMR measurements

Claim 1

A method of gyromagnetic resonance spectroscopy operative upon an assembly of gyromagnetic resonators immersed in a polarizing magnetic field, said field directed along a first axis, wherein the magnetization vectors of said gyromagnetic resonators precess about said polarizing magnetic field, comprising the steps of (a) tipping the magnetic vectors 90° from said first axis, said tipping accomplished by rotating said magnetic vector about a second axis, said second axis orthogonal to said first axis and said rotation of selected sense, whereby said magnetic vectors rotate in a plane orthogonal to said first axis, (b) permitting the progressive loss of phase coherence among said rotating magnetic vectors for an interval of time T, (c) reversing the sense of rotation of said magnetic vectors by inverting the sense of said first axis through rotation of 180° with respect to said first axis, whereby said progressive loss of phase coherence is reversed, (d) permitting the progressive approach to phase coherence among said rotating magnetic vectors, (e) detecting a spin echo resonance signal of said resonators, said signal possibly containing transients of instrumental origin arising from steps (a) and (c), (f) storing said resonance signal, (g) repeating the steps (a) and (b) and inverting the sense of said first axis by rotating said coordinate systems through 180° with respect to said first axis, said rotation accomplished about said second axis, said rotation sense opposite said selected sense and repeating the steps (d) through (e), (h) adding the signal stored in step (f) with the signal detected in step (g) to form a cumulative signal free of transients arising from said 180° rotations of steps (c) and reinversion of step (g), (i) repeating steps (a) and (b) and inverting the sense of said first axis by rotation of said magnetic vector about a third axis, said axis orthogonal to said first and second axes and said 180° rotation having second selected sense whereby said loss of phase coherence is reversed and repeating again steps (d) and (e), (j) subtracting the signal detected in step (i) from the cumulative signal obtained at step (h) and storing said cumulative signal, (k) repeating steps (a) and (b) and inverting the sense of said first axis by rotation of said magnetic vector through 180° about said third axis, said 180° rotation in sense opposite said second selected sense and repeating steps (d) through (e), (l) subtracting the signal detected in step (k) from said cumulative signal obtained and stored at step (j) and storing said new cumulative signal, whereby ringing incident to step (a) repeated at step (g) is canceled against the ringing experienced at steps (i) and (k).

Claim 2

A method of gyromagnetic resonance spectroscopy operative upon an assembly of gyromagnetic resonators immersed in a polarizing magnetic field, said field directed along a first axis, wherein the magnetization vectors of said gyromagnetic resonators precess about said polarizing magnetic field, comprising the steps of (a) tipping the magnetic vectors 90° from said first axis, said tipping accomplished by rotating said magnetic vector about a second axis, said second axis orthogonal to said first axis and said rotation of selected sense, whereby said magnetic vectors rotate in a plane orthogonal to said first axis, (b) permitting the progressive loss of phase coherence among said rotating magnetic vectors for an interval of time T, (c) reversing the sense of rotation of said magnetic vectors by inverting the sense of said first axis through rotation of 180° with respect to said first axis, whereby said progressive loss of phase coherence is reversed, (d) permitting the progressive approach to phase coherence among said rotating magnetic vectors, (e) detecting a spin echo resonance signal of said resonators, said signal possibly containing transients of instrumental origin arising from steps (a) and (c), (f) storing said resonance signal, (g) repeating the steps (a) and (b) and inverting the sense of said first axis by rotating said coordinate systems through 180° with respect to said first axis, said rotation accomplished about said second axis, said rotation sense opposite said selected sense and repeating the steps (d) through (e), (h) adding the signal stored in step (f) with the signal detected in step (g) to form a cumulative signal free of transients arising from said 180° rotations of steps (c) and reinversion of step (g), (i) repeating steps (a) and (b) and inverting the sense of said first axis by rotation of said magnetic vector about a third axis, said axis orthogonal to said first and second axes and said 180° rotation having second selected sense whereby said loss of phase coherence is reversed and repeating again steps (d) and (e), (j) subtracting the signal detected in step (i) from the cumulative signal obtained at step (h) and storing said cumulative signal, (k) repeating steps (a) and (b) and inverting the sense of said first axis by rotation of said magnetic vector through 180° about said third axis, said 180° rotation in sense opposite said second selected sense and repeating steps (d) through (e), (l) subtracting the signal detected in step (k) from said cumulative signal obtained and stored at step (j) and storing said new cumulative signal, whereby ringing incident to step (a) repeated at step (g) is canceled against the ringing experienced at steps (i) and (k).

Claim 3

A method of gyromagnetic resonance spectroscopy operative upon an assembly of gyromagnetic resonators immersed in a polarizing magnetic field oriented along a first axis wherein the magnetization vectors of said gyromagnetic resonators precess about said polarizing magnetic field comprising the steps of (a) rotating said magnetization vectors through a selected angle with respect to said first axis, said rotation carried out in selected sense about a second axis orthogonal said first axis, (b) permitting the progressive loss of phase coherence among said gyromagnetic resonators for interval of time T, (c) inverting the sense of said first axis by rotating the system 180° with respect to said first axis, said rotation carried out and accompanied by ringing, (d) permitting the increase of phase coherence among said gyromagnetic resonators for another interval of time, (e) repeating step (c), (f) detecting the double spin echo resonance of said resonators whereby the magnetization component remaining along said first axis after step (a) and inverted by step (e) is restored to the initial orientation thereof, (g) said rotation of step (c), phase cycled among phases of 90° separation in subsequent repetition of steps (a) through (f).

Claim 4

A method of gyromagnetic resonance spectroscopy operative upon an assembly of gyromagnetic resonators immersed in a polarizing magnetic field oriented along a first axis wherein the magnetization vectors of said gyromagnetic resonators precess about said polarizing magnetic field comprising the steps of (a) rotating said magnetization vectors through a selected angle with respect to said first axis, said rotation carried out in selected sense about a second axis orthogonal said first axis, (b) permitting the progressive loss of phase coherence among said gyromagnetic resonators for interval of time T, (c) inverting the sense of said first axis by rotating the system 180° with respect to said first axis, said rotation carried out and accompanied by ringing, (d) permitting the increase of phase coherence among said gyromagnetic resonators for another interval of time, (e) repeating step (c), (f) detecting the double spin echo resonance of said resonators whereby the magnetization component remaining along said first axis after step (a) and inverted by step (e) is restored to the initial orientation thereof, (g) said rotation of step (c), phase cycled among phases of 90° separation in subsequent repetition of steps (a) through (f).

Claim 5

A method of magnetic resonance spectroscopy of gyromagnetic resonators comprising (a) polarizing the magnetic vectors of said resonators about the polarization axis whereby the vectors representative of said resonators precess about said polarization axis, (b) coherently tipping said magnetic vectors through a desired angle with respect to said polarization axis, (c) detecting and storing a resulting first resonance signal, (d) delaying for a fixed interval of time, (e) inverting said magnetization vectors 180° with respect to the direction of polarization, (f) again coherently tipping said magnetic vector through said desired angle with respect to said polarization axis and obtaining a second resonance signal, (g) subtracting said second signal from said first signal to form a cumulative signal and storing said cumulative signal whereby the nonresonant portions of said signal accompanying said steps of coherent tipping and again coherent tipping will cancel, while resonant portions of said signals add.

Claim 6

A method of magnetic resonance spectroscopy of gyromagnetic resonators comprising (a) polarizing the magnetic vectors of said resonators about the polarization axis whereby the vectors representative of said resonators precess about said polarization axis, (b) coherently tipping said magnetic vectors through a desired angle with respect to said polarization axis, (c) detecting and storing a resulting first resonance signal, (d) delaying for a fixed interval of time, (e) inverting said magnetization vectors 180° with respect to the direction of polarization, (f) again coherently tipping said magnetic vector through said desired angle with respect to said polarization axis and obtaining a second resonance signal, (g) subtracting said second signal from said first signal to form a cumulative signal and storing said cumulative signal whereby the nonresonant portions of said signal accompanying said steps of coherent tipping and again coherent tipping will cancel, while resonant portions of said signals add.