WO2013027710A1 - 磁気共鳴イメージング装置および補正値算出方法 - Google Patents
磁気共鳴イメージング装置および補正値算出方法 Download PDFInfo
- Publication number
- WO2013027710A1 WO2013027710A1 PCT/JP2012/071020 JP2012071020W WO2013027710A1 WO 2013027710 A1 WO2013027710 A1 WO 2013027710A1 JP 2012071020 W JP2012071020 W JP 2012071020W WO 2013027710 A1 WO2013027710 A1 WO 2013027710A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- phase difference
- magnetic field
- calculation unit
- gradient magnetic
- excitation
- Prior art date
Links
Images
Classifications
-
- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61B—DIAGNOSIS; SURGERY; IDENTIFICATION
- A61B5/00—Measuring for diagnostic purposes; Identification of persons
- A61B5/05—Detecting, measuring or recording for diagnosis by means of electric currents or magnetic fields; Measuring using microwaves or radio waves
- A61B5/055—Detecting, measuring or recording for diagnosis by means of electric currents or magnetic fields; Measuring using microwaves or radio waves involving electronic [EMR] or nuclear [NMR] magnetic resonance, e.g. magnetic resonance imaging
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R33/00—Arrangements or instruments for measuring magnetic variables
- G01R33/20—Arrangements or instruments for measuring magnetic variables involving magnetic resonance
- G01R33/44—Arrangements or instruments for measuring magnetic variables involving magnetic resonance using nuclear magnetic resonance [NMR]
- G01R33/48—NMR imaging systems
- G01R33/54—Signal processing systems, e.g. using pulse sequences ; Generation or control of pulse sequences; Operator console
- G01R33/56—Image enhancement or correction, e.g. subtraction or averaging techniques, e.g. improvement of signal-to-noise ratio and resolution
- G01R33/561—Image enhancement or correction, e.g. subtraction or averaging techniques, e.g. improvement of signal-to-noise ratio and resolution by reduction of the scanning time, i.e. fast acquiring systems, e.g. using echo-planar pulse sequences
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R33/00—Arrangements or instruments for measuring magnetic variables
- G01R33/20—Arrangements or instruments for measuring magnetic variables involving magnetic resonance
- G01R33/44—Arrangements or instruments for measuring magnetic variables involving magnetic resonance using nuclear magnetic resonance [NMR]
- G01R33/48—NMR imaging systems
- G01R33/4816—NMR imaging of samples with ultrashort relaxation times such as solid samples, e.g. MRI using ultrashort TE [UTE], single point imaging, constant time imaging
Definitions
- the present invention measures a nuclear magnetic resonance signal (hereinafter referred to as an NMR signal) from hydrogen, phosphorus, etc. in a subject and images a nuclear density distribution, relaxation time distribution, etc. (hereinafter referred to as MRI).
- NMR signal nuclear magnetic resonance signal
- MRI nuclear density distribution, relaxation time distribution, etc.
- the present invention relates to an imaging technique using an ultrashort echo time sequence.
- the MRI device measures NMR signals (echo signals) generated by the spins of the subject, especially the tissues of the human body, and forms the shape and function of the head, abdomen, limbs, etc. in two or three dimensions. It is a device that images.
- NMR signals echo signals
- the subject is placed in a static magnetic field (polarization magnetic field B0), and a slice selective gradient magnetic field pulse is applied together with a high-frequency magnetic field pulse (RF pulse) to selectively excite a specific region, and a phase encoding gradient is applied.
- RF pulse high-frequency magnetic field pulse
- the slice gradient magnetic field pulse generates a magnetic field inclined in an arbitrary direction, and generates a magnetic field strength gradient in the static magnetic field space.
- the nuclear spin constituting the object precesses at a frequency corresponding to the strength of the tilted magnetic field and the gyromagnetic ratio.
- the frequency of the precession is called the Larmor frequency.
- excitation profile In the ideal state ignoring the relaxation phenomenon of nuclear spins, this excited range and intensity (hereinafter referred to as excitation profile) are in the form of Fourier transform of the RF pulse envelope.
- the most common waveform of an RF pulse envelope is the Sinc function.
- Sinc function When the Sinc function is used for the envelope of the RF pulse, a rectangular excitation profile can be obtained except for truncation errors.
- Photographing is performed according to a predetermined pulse sequence.
- the pulse sequences there is an ultra-short echo time sequence (Ultra-short TE Sequence; hereinafter referred to as UTE sequence) for measuring a tissue signal with a short transverse relaxation time (T2) (Patent Document 1, Non-Patent Document). 1).
- UTE sequence a half RF pulse (Half RF pulse) in which the waveform of a normal RF pulse (full RF pulse: Full RF pulse) is halved is used as the envelope of the RF pulse.
- each half RF pulse is irradiated with a slice gradient magnetic field whose polarity is reversed, excitation is performed twice, and echo signals are measured and added twice in association with excitation.
- the slice gradient magnetic field to be applied with the polarity as the positive polarity is the positive slice gradient magnetic field
- the slice gradient magnetic field to be applied with the polarity as the negative polarity is the negative slice gradient magnetic field
- the echo signal acquired when the positive slice gradient magnetic field is applied.
- An echo signal acquired when positive data and a negative slice gradient magnetic field are applied is referred to as negative data.
- the half RF pulse excitation profile has a larger sidelobe than the full RF pulse excitation profile.
- the excitation profile of the positive and negative data has a phase distribution that is inverted by 180 [deg] in the side lobe, adding the positive and negative data cancels the side lobe signal.
- An excitation profile equivalent to the excitation profile by the RF pulse can be obtained.
- the side lobe signal of the excitation profile is canceled by adding the positive data and the negative data.
- the excitation profiles of the positive electrode data and the negative electrode data do not actually have a phase distribution inverted by 180 [deg] in the side lobe portion.
- the side lobe signals of the positive data and the negative data are not canceled out, signals from outside the designated slice position are mixed in the reconstructed image, resulting in artifacts and a good image cannot be obtained.
- the present invention has been made in view of the above circumstances, and an object thereof is to obtain a high-quality image by a UTE sequence.
- the present invention adjusts the refocusing pulse of the slice gradient magnetic field so that the excitation profiles of the positive electrode data and the negative electrode data acquired by applying the half RF pulse have a phase distribution inverted by 180 [deg] in the side lobe part.
- a good excitation profile is realized in the UTE sequence.
- a high-quality image can be obtained regardless of the number of slices in the UTE sequence.
- Pulse sequence diagram of UTE sequence This is an excitation profile (intensity distribution) of a half RF pulse, and is an explanatory diagram for explaining that side lobes in the excitation profile of a half RF pulse are reduced by adding positive and negative data Explanatory diagram for explaining that the excitation profile (phase distribution) of the half RF pulse has a phase distribution in which the excitation profile of the positive and negative data is inverted by 180 [deg] in the side lobe portion.
- Explanatory drawing explaining the magnetic field generated by eddy current distorts the output gradient magnetic field waveform Explanatory drawing for explaining the application timing of the RF pulse and slice gradient magnetic field when irradiating a half RF pulse using the downward part of the slice gradient magnetic field (a) illustrates the displacement of the excitation position when an offset occurs in the positive electrode slice gradient magnetic field, and (b) illustrates the displacement of the excitation position when an offset occurs in the negative electrode slice gradient magnetic field.
- Illustration of Functional block diagram of the arithmetic system of the first embodiment (a) and (b) are explanatory diagrams for explaining the measurement results of the positive electrode slice gradient magnetic field waveform and the negative electrode slice gradient magnetic field waveform of the first embodiment, respectively.
- (a) is an explanatory diagram for explaining the phase distribution after the phase difference between the positive electrode data and the negative electrode data of the second embodiment
- (b) is a phase unwrap process on the data shown in (a) Explanatory diagram for explaining the later phase Flow chart of pre-processing of the second embodiment
- (a)-(g) is explanatory drawing for demonstrating the improvement effect of the excitation profile at the time of using the correction value of 2nd embodiment.
- (a)-(d) is explanatory drawing for demonstrating the image improvement effect at the time of using the correction value of 2nd embodiment.
- FIG. 1 is a block diagram showing the overall configuration of the MRI apparatus 100 of the present embodiment.
- the MRI apparatus 100 of the present embodiment obtains a tomographic image of a subject using an NMR phenomenon, a static magnetic field generation system 120, a gradient magnetic field generation system 130, a sequencer 140, a high-frequency magnetic field generation system 150, A high-frequency magnetic field detection system 160 and a calculation system 170 are provided.
- the static magnetic field generation system 120 generates a uniform static magnetic field in the direction perpendicular to the body axis in the space around the subject 101 if the vertical magnetic field method is used, and in the direction of the body axis if the horizontal magnetic field method is used.
- a permanent magnet type, normal conducting type or superconducting type static magnetic field generating source is arranged around the subject 101.
- the gradient magnetic field generation system 130 is a gradient magnetic field coil 131 wound in the three-axis directions of X, Y, and Z, which is the coordinate system (stationary coordinate system) of the MRI apparatus 100, and the gradient magnetic field that drives each gradient magnetic field coil 131.
- a gradient magnetic field Gxin, Gyin, Gzin is applied to the three axes of X, Y, and Z by driving the gradient magnetic field power supply 132 of each coil in accordance with a command from a sequencer 140 described later. .
- a slice direction gradient magnetic field pulse is applied in a direction orthogonal to the slice plane (imaging cross section) to set a slice plane for the subject 101, and the remaining planes orthogonal to the slice plane and orthogonal to each other are set.
- a phase encoding direction gradient magnetic field pulse (Gp) and a frequency encoding direction gradient magnetic field pulse (Gf) are applied in two directions, and position information in each direction is encoded into an NMR signal (echo signal).
- the high-frequency magnetic field generation system 150 irradiates the subject 101 with an RF pulse in order to cause nuclear magnetic resonance to occur in the nuclear spins of atoms constituting the biological tissue of the subject 101, and modulates with the high-frequency oscillator (synthesizer) 152. 153, a high frequency amplifier 154, and a high frequency coil (transmission coil) 151 on the transmission side.
- the high-frequency pulse output from the synthesizer 152 is amplitude-modulated by the modulator 153 at a timing according to a command from the sequencer 140, and the amplitude-modulated high-frequency pulse is amplified by the high-frequency amplifier 154 and arranged close to the subject 101.
- the transmission coil 151 the subject 101 is irradiated with the RF pulse.
- the high-frequency magnetic field detection system 160 detects an echo signal (NMR signal) emitted by nuclear magnetic resonance of nuclear spins constituting the living tissue of the subject 101.
- An amplifier 162, a quadrature detector 163, and an A / D converter 164 are provided.
- the echo signal of the response of the subject 101 induced by the electromagnetic wave irradiated from the transmission coil 151 is detected by the reception coil 161 arranged close to the subject 101, amplified by the signal amplifier 162, and then from the sequencer 140.
- the sequencer 140 is a control unit that repeatedly applies a high-frequency magnetic field pulse (hereinafter referred to as “RF pulse”) and a gradient magnetic field pulse according to a predetermined imaging sequence.
- the sequencer 140 operates under the control of the arithmetic system 170 and sends various commands necessary for collecting tomographic image data of the subject 101 to the gradient magnetic field generation system 130, the high-frequency magnetic field generation system 150, and the high-frequency magnetic field detection system 160.
- These gradient magnetic field generation system 130, high-frequency magnetic field generation system 150, and high-frequency magnetic field detection system 160 operate in accordance with instructions from sequencer 140 and perform measurement, and are collectively referred to as a measurement system.
- the arithmetic system 170 performs various data processing, display and storage of processing results, and includes a CPU 171, a storage device 172, an external storage device 173, a display device 174, and an input device 175.
- the tomographic image of the subject 101 is reconstructed using data from the high-frequency magnetic field detection system 160. Further, a control signal is transmitted to the sequencer 140 in accordance with the photographing sequence.
- the reconstructed tomographic image is displayed on the display device 174 and recorded in the storage device 172 or the external storage device 73.
- the input device 175 is used by an operator to input various control information of the MRI apparatus 100 and control information of processing performed by the arithmetic system 170, and includes a trackball or a mouse and a keyboard.
- the input device 175 is disposed in the vicinity of the display device 174, and an operator controls various processes of the MRI apparatus 100 interactively through the input device 175 while looking at the display device 174.
- the transmission coil 151 and the gradient magnetic field coil 131 are arranged in a static magnetic field space of the static magnetic field generation system 20 into which the subject 101 is inserted, and face the subject 101 in the vertical magnetic field system, If the magnetic field method is used, it is installed so as to surround the subject 101. Further, the receiving coil 161 is installed so as to face or surround the subject 101.
- the radionuclide to be imaged by the MRI apparatus is a hydrogen nucleus (proton), which is the main constituent material of the subject, as widely used in clinical practice.
- proton the main constituent material of the subject
- the form or function of the human head, abdomen, limbs, etc. is imaged two-dimensionally or three-dimensionally.
- the imaging sequence from which the CPU 171 of the arithmetic system 170 gives the control signal to the sequencer 140 includes the pulse sequence in which the application timing of the RF pulse and the gradient magnetic field pulse is determined, the application intensity of the RF pulse and the gradient magnetic field pulse, the application timing, etc. Determined by the parameter to be specified.
- the pulse sequence is preset and held in the storage device 172.
- the parameters are calculated in the arithmetic system 170 based on the shooting conditions set by the operator via the input device 175.
- a pulse sequence of the UTE sequence 200 is shown in FIG.
- the horizontal axes in FIG. 2 are all time axes [s]
- the vertical axes of RF and Echo are voltage amplitudes [V]
- the vertical axes of Gs, Gp, and Gf are gradient magnetic field strengths [T / m].
- the slice gradient magnetic field 211 and the slice gradient magnetic field 212 are applied with their polarities reversed.
- the slice gradient magnetic field applied with the polarity as the positive electrode is referred to as a positive electrode slice gradient magnetic field
- the slice gradient magnetic field applied with the polarity as the negative electrode is referred to as a negative electrode slice gradient magnetic field.
- the echo signals 241 and 242 are measured while applying the phase encode gradient magnetic fields 221 and 222 and the read encode gradient magnetic fields 231 and 232, respectively.
- the echo signal 241 acquired by applying the positive slice magnetic gradient 211 is referred to as positive data
- the echo signal 242 acquired by applying the negative slice gradient 212 is referred to as negative data.
- the arithmetic system 170 reconstructs an image after adding the measured echo signals 241 and 242 to each other.
- the excitation profile of the half RF pulse has a larger side lobe than the excitation profile of the full RF pulse, but an excitation profile equivalent to that of the full RF pulse can be obtained by addition.
- FIG. 3 shows an excitation profile 303 of data obtained by adding excitation profiles 301 and 302 by half RF pulses 201 and 202, respectively, and positive and negative data obtained from half RF pulses 201 and 202 in UTE sequence 200.
- the horizontal axis represents the position (Position [m])
- the vertical axis represents the intensity (Amplitude [a.u.]).
- An excitation profile 303 equivalent to a full RF pulse can be obtained by adding echo signals. This reason can be explained from the phase distribution of the excitation profile by the half RF pulse.
- FIG. 4 shows the phase distributions 311 and 312 of the excitation profiles by the half RF pulses 201 and 202, respectively.
- the horizontal axis in FIG. 4 represents the position (Position [m]), and the vertical axis represents the phase (Phase [deg]).
- the phase distribution 311 of the excitation profile 301 obtained by the positive electrode slice gradient magnetic field 211 and the phase distribution 312 of the excitation profile 302 obtained by the negative electrode slice gradient magnetic field 212 are 180 [deg] in the side lobe portion.
- the relationship is reversed. Therefore, when the data (positive data and negative data) obtained by both are added, a phase distribution 313 in which the side lobe signal is canceled is obtained.
- phase distribution of the excitation profile of the positive electrode data and the phase distribution of the excitation profile of the negative electrode data do not actually have a 180 [deg] inverted relationship.
- a positional deviation occurs between the intensity distribution of the positive electrode data and the intensity distribution of the negative electrode data.
- phase distribution of the positive and negative data is not reversed by 180 [deg] is the eddy current generated by the slice gradient magnetic field and the relaxation during irradiation of the half RF pulses 201 and 202.
- FIG. 5 is a conceptual diagram showing the state of the slice gradient magnetic field waveform 322 that has changed due to the generation of eddy currents relative to the slice gradient magnetic field waveform 321 specified by the imaging parameters.
- relaxation during half RF pulses 201 and 202 causes phase dispersion of nuclear spins and changes the phase distribution of the excitation profile.
- the influence of relaxation appears remarkably. This lowers the irradiation intensity of the half RF pulses 201 and 202 in accordance with the intensity of the slice gradient magnetic fields 211 and 212, and the flip angle of the nuclear spin is reduced and the irradiation time is extended in the portion where the irradiation intensity is reduced. Because.
- the cause of the positional deviation in the intensity distribution of the positive and negative data is the offset component of the slice gradient magnetic fields 211 and 212.
- the excited position is shifted in proportion to the offset.
- the shift is in the opposite direction between the case where the slice gradient magnetic field is positive and the case where the negative electrode is negative. Therefore, the intensity distributions of both do not match, and when both are added, the width of the main lobe increases and the side lobe signal remains. .
- FIGS. 7 (a) and 7 (b) are diagrams for explaining how the position 342 to be excited is shifted in proportion to the offset 343 from the position 341 to be excited when the slice gradient magnetic field has an offset.
- FIG. FIG. 7 (a) shows a case where the slice gradient magnetic field is a positive electrode (positive electrode slice gradient magnetic field 211).
- FIG. 7 (b) shows the case where the slice gradient magnetic field is a negative electrode (negative electrode slice gradient magnetic field 212).
- the actually excited position 342 shifts in the opposite direction. Therefore, the intensity distributions of the two do not match, and when the two are added, the width of the main lobe becomes wide and the side lobe signal remains.
- This side lobe signal can be suppressed by applying a saturation pulse (Saturation Pulse) so as to be adjacent to the slice plane.
- a saturation pulse Saturation Pulse
- the waveform of the slice gradient magnetic fields 211 and 212 is measured, a correction value is calculated from the result, and the pulse sequence and the reconstruction process are changed using the correction value.
- Processing by the arithmetic system 170 of this embodiment is roughly divided into two.
- the first process is a pre-process for calculating correction values used for the pulse sequence and the reconstruction process from the measurement results of the slice gradient magnetic fields 211 and 212.
- the correction values calculated in the preprocessing are: 1) Refocus area of slice gradient magnetic field (amount of refocus pulse applied to slice gradient magnetic fields 211 and 212), 2) Irradiation frequency of half RF pulses 201 and 202, 3) Positive electrode data And zero-order term (zero-order phase difference) of the phase difference between the negative electrode data and the negative electrode data.
- the second process reflects the calculated refocus pulse application amount and irradiation frequency in the UTE sequence 200, changes the UTE sequence 200, performs measurement, and reconstructs it by reflecting the zeroth-order phase difference. This is the main measurement process.
- the arithmetic system 170 of this embodiment includes a pre-processing unit 710 and a main measurement unit 720 as shown in FIG.
- the pre-processing unit 710 includes a slice gradient magnetic field waveform measurement unit 711, a refocus pulse application amount calculation unit 712, an irradiation frequency calculation unit 713, and a zero-order phase difference calculation unit 714.
- the main measurement unit 720 includes an image reconstruction unit 721.
- Any function of the arithmetic type 170 is realized by the CPU 171 of the arithmetic system 170 loading a program stored in the storage device 172 or the external storage device 173 in advance into the memory and executing it. This is the same for all embodiments described later.
- the slice gradient magnetic field waveform measuring unit 711 measures the slice gradient magnetic field waveform actually applied at each slice position. The measurement is performed using a known technique. In the UTE sequence 200, when the slice gradient magnetic fields 211 and 212 are applied according to the imaging parameters, an output slice gradient magnetic field waveform is determined.
- Non-Patent Document 2 when the method described in Non-Patent Document 2 is used, the measurement is performed as follows.
- a slice gradient magnetic field for measuring the waveform is set as a test gradient magnetic field. After exciting a given thin slice, a test gradient magnetic field was applied according to the imaging parameters and a signal was acquired, and a reference sequence was acquired without applying the test gradient magnetic field.
- the gradient magnetic field output waveform of the test gradient magnetic field is measured by calculation between signals.
- the respective waveforms of the positive electrode slice gradient magnetic field 211 and the negative electrode slice gradient magnetic field 212 are measured.
- the obtained positive electrode slice gradient magnetic field waveform is Waveform_positive (x)
- the negative electrode slice gradient magnetic field waveform is Waveform_negative (x).
- x represents a discrete point number representing a position in the slice direction.
- FIG. 9 (a) illustrates Waveform_positive (x) 411
- FIG. 9 (b) illustrates Waveform_negative (x) 412.
- a waveform when there is a gradient magnetic field offset GcOffset is shown.
- RF_Start_Time is the application start time of the half RF pulses 201 and 202, respectively.
- RF_End_Time is the application end time of the half RF pulses 201 and 202, respectively.
- the slice gradient magnetic field that is actually applied is distorted from a rectangular shape, and is also applied after the end of half-RF pulse application (RF_End_Time).
- the refocus pulse application amount calculation unit 712 calculates the refocus pulse application amount of each of the positive slice gradient magnetic field 211 and the negative slice gradient magnetic field 212 as a correction value at each slice position.
- the gradient magnetic field generated by is applied.
- the refocus pulse is an area adjustment pulse applied to cancel the gradient magnetic field application amount (the surplus application amount of the slice gradient magnetic field) during this period.
- the refocus pulses 251 and 252 are applied immediately after the slice gradient magnetic fields 211 and 212 are applied, as shown in FIG.
- the refocus pulse application amount calculation unit 712 of the present embodiment calculates surplus application amounts of the slice gradient magnetic fields 211 and 212 using the measured slice gradient magnetic field waveforms Waveform_positive (x) 411 and Waveform_negative (x) 412. The application amount is determined so as to cancel it.
- the refocus pulse application amount calculation unit 712 of the present embodiment calculates the application amount (area) of the refocus pulse 251 by the following equations (1) and (2).
- Adjust_Area_251 is the surface [s ⁇ T / m] of the refocus pulse 251
- Adjust_Area_252 is the area [s ⁇ T / m] of the refocus pulse 252
- RF_End_Time is the irradiation end time [s of the half RF pulses 201 and 202]
- TE is the time from the irradiation end time of the half RF pulses 201, 202 to the acquisition of the respective echo signals 241, 242.
- the irradiation frequency calculation unit 713 calculates the irradiation frequency of the half RF pulses 201 and 202 irradiated at each slice position as a correction value. If there is a displacement of the excitation position between the positive slice gradient magnetic field 211 and the negative slice gradient magnetic field 212 according to the obtained slice gradient magnetic field waveform, the irradiation frequency calculation unit 713 of the present embodiment calculates the displacement. Each irradiation frequency is decided so that it may eliminate. The excitation position deviation is calculated from the actually measured intensities of the measured slice gradient magnetic fields 211 and 212.
- the irradiation frequency calculation unit 713 of the present embodiment includes the irradiation frequency Frequency_Positive [Hz] of the half RF pulse 201 applied together with the positive slice gradient magnetic field 211 and the half RF pulse 202 applied together with the positive slice gradient magnetic field 212.
- the irradiation frequency Frequency_Nagative [Hz] is determined using the determined waveform Waveform_positive (x) of the slice gradient magnetic field 211 and the waveform Waveform_negative (x) of the slice gradient magnetic field 212, respectively, according to the following equations (3) and (4): calculate.
- ⁇ is the magnetic rotation ratio [Hz / T]
- GcAmp1 is the measured intensity [T / m] of the positive electrode slice gradient magnetic field 211 (the plateau portion of the measured waveform 411 of the positive electrode slice gradient magnetic field 211 shown in FIG. 9 (a)). Intensity)
- GcAmp2 is the measured intensity [T / m] of the negative slice gradient magnetic field 212 (the intensity of the plateau part of the measured waveform 412 of the negative slice gradient magnetic field 412 shown in FIG. 9B)
- Offcenter is the specified slice position from the magnetic field center.
- GmBase is the static magnetic field strength [T].
- the 0th-order phase difference calculation unit 714 calculates the value of the 0th-order term (0th-order phase difference) of the difference between the phase of the acquired positive electrode data and the negative electrode data at each slice position as a correction value.
- the 0th-order phase difference calculation unit 714 of the present embodiment calculates the 0th-order phase difference using the measured waveform of the positive electrode slice gradient magnetic field 211 and the measured waveform of the negative electrode slice gradient magnetic field 212 using the following equation (5). .
- ZerothOrderPhase is 0th-order phase difference [deg]
- RF_Start_Time is irradiation start time [s] of half RF pulses 201 and 202
- Offcenter is a distance [m] from the magnetic field center to the specified slice position
- ⁇ x is Waveform_positive Sampling interval [s] between () and Waveform_negative ().
- Expression (5) is an expression for calculating the phase shift of the negative electrode data with respect to the positive electrode data.
- Waveform_positive (x) and Waveform_negative (y) may be reversed to calculate the phase shift of the positive data with respect to the negative data.
- the main measurement unit 720 of this embodiment sets the refocus pulse application amount and the irradiation frequency calculated as correction values by the refocus pulse application amount calculation unit 712 and the irradiation frequency calculation unit 713, respectively, in the UTE sequence 200, and performs the main measurement. Execute.
- the image reconstruction unit 721 adds positive electrode data and negative electrode data obtained by this measurement, and reconstructs an image from the data obtained by the addition (polarity addition data) using a known method such as Fourier transform. .
- the phase difference between the positive electrode data and the negative electrode data is corrected using the zeroth-order phase difference before the addition.
- the phase shift of the negative electrode data with respect to the positive electrode data is calculated as the zeroth-order phase difference (in the case of the above formula (5)) will be described as an example.
- the 0th-order phase difference calculated by the equation (5) is added to the negative electrode data according to the following equations (6) and (7).
- Main_negative (real,) and Main_negative (imagn,) are the real part and imaginary part of the negative data before the zero-order phase addition, respectively, Main_negative '(real,) and Main_negative' (imagn,) are respectively The real part and imaginary part of the negative electrode data after addition of the 0th-order phase, and ZerothOrderPhase are the 0th-order phase difference [deg] calculated by Expression (5).
- Main_positive (real,) and Main_positive (imagn,) are the real part and imaginary part of the positive data before the 0th-order phase addition, respectively, Mian_composed (real,) and Mian_composed (imagn,) are the polarity addition, respectively.
- the real and imaginary parts of the data are the real part and imaginary parts of the data.
- the zero-order phase difference is calculated as the phase shift of the positive electrode data with respect to the negative electrode data
- the zero-order phase difference is added to the positive data side by the above method, and then the positive and negative data after the addition Is added.
- FIG. 11 is a processing flow showing the flow of pre-processing in the present embodiment.
- the preprocessing unit 710 performs preprocessing for calculating a correction value for each slice.
- the total number of slices is N.
- the pre-processing unit 710 repeats the processing from step S1102 to step S1106 through repetitive processing (step S1101 and step S1107).
- the number of repetitions is the number of slices (N in this case) specified as the imaging condition for the main measurement.
- i represents the slice number to be processed during the repeated processing.
- the slice gradient magnetic field waveform measurement unit 711 measures the waveform of the positive electrode slice gradient magnetic field 211 at the i-th slice position (step S1102), and then measures the waveform of the negative electrode slice gradient magnetic field 212 (step S1103). Note that either of the measurement of the waveforms of the slice gradient magnetic fields 211 and 212 may be first.
- the refocus pulse application amount calculation unit 712 uses the measured waveform of the positive slice gradient magnetic field 211 and the measured waveform of the negative slice gradient magnetic field 212 to refocus pulses 251 for each slice gradient magnetic field at the i-th slice position,
- the application amount of 252 is calculated by the above formulas (1) and (2), respectively (step S1104).
- the irradiation frequency calculation unit 713 uses the measured waveform of the positive electrode slice gradient magnetic field 211 and the measured waveform of the negative electrode slice gradient magnetic field 212, and calculates the irradiation frequency of each half RF pulse 201, 202 at the i-th slice position as described above. Calculations are made according to equations (3) and (4), respectively (step S1105).
- the zero-order phase determination unit uses the measured waveform of the positive slice gradient magnetic field 211 and the measured waveform of the negative slice gradient magnetic field 212, and uses the zero-order phase difference between the positive and negative data at the i-th slice position. Is calculated by the above equation (5) (step S1106).
- the arithmetic system 170 performs pre-processing, and calculates the correction values of the irradiation frequencies of the half RF pulses 201 and 202, the application amounts of the refocus pulses 251 and 252 and the zero-order phase difference.
- step S1102 any of the processes of S1103, S1104, and S1105 may be performed first.
- FIG. 12 is a process flow of the main measurement process of the present embodiment.
- the main measurement unit 720 first generates a pulse sequence used for the main measurement by using the set imaging parameter and the correction value determined by the pre-processing (step S1201).
- the determined irradiation frequency and refocus pulse application amount for each slice are reflected in the UTE sequence 200 shown in FIG.
- the main measurement unit 720 issues an instruction to the sequencer 140 according to the generated UTE sequence 200, performs measurement, and acquires positive electrode data and negative electrode data (step S1202).
- the image reconstruction unit 721 adds the 0th-order phase difference calculated in the preprocessing to the negative electrode data (Step S1203). Then, the image reconstruction unit 721 adds the positive electrode data and the negative electrode data after the addition (step S1204) to obtain polarity addition data.
- the main measurement unit 720 repeats the processing from step S1202 to S1204 until it is determined that the measurement is finished (step S1205).
- the determination of the end of measurement is determined in advance. For example, when the number of acquired echoes satisfies the specified number, or when an instruction to interrupt the process is received, it is determined that the measurement is finished.
- the image reconstruction unit 721 reconstructs an image from the polarity addition data (step S1206) and outputs the image to the display device 174, the storage device 172, the external storage device 173, and the like (step S1207).
- the number of repetitions is the number of slices N set in the shooting conditions, but is not limited thereto.
- all slice positions that can be imaged by the MRI apparatus 100 may be designated, and the number of positions may be repeated.
- the irradiation frequency calculation process is performed when there is a deviation in the excitation position between the positive electrode data and the negative electrode data. In the case of an MRI apparatus in which the excitation position is unlikely to shift, the calculation of the irradiation frequency may not be performed. In this case, the irradiation frequency calculation unit 713 may not be provided.
- the main measurement unit 720 sets the irradiation frequency set by the imaging parameter or the irradiation frequency obtained by a known technique in the UTE sequence 200.
- the 0th-order phase difference calculation unit 714 may not be provided.
- the zero-order phase difference is not calculated, for example, 0 [deg] is set as the phase difference, either the negative data before addition by the image reconstruction unit 721 or the positive data is not corrected, etc. It is good also as a structure.
- the measurement system includes the static magnetic field generation system 120, the gradient magnetic field generation system 130, the high-frequency magnetic field generation system 150, and the high-frequency magnetic field detection system 160, and the measurement system according to the pulse sequence.
- a magnetic resonance imaging apparatus comprising: an operation system 170 that controls the operation of the magnetic resonance signal to measure a nuclear magnetic resonance signal and performs an operation using data obtained from the nuclear magnetic resonance signal.
- This is an ultra-short echo time sequence in which the slice gradient magnetic field applied together with the RF pulse is inverted between the positive and negative electrodes to perform two slice selective excitations to obtain echo signals, respectively.
- a pre-processing unit 710 that calculates a correction value used for the calculation, and the correction value calculated by the pre-processing unit 710 is set in the pulse sequence
- a main measurement unit 720 that controls the measurement system according to a pulse sequence to perform main measurement and reconstructs an image, and the pre-processing unit 710 determines an application amount of a refocus pulse of each slice gradient magnetic field.
- Refocusing pulse application amount calculation unit 712 for calculating each as the correction value and the main measurement unit 720 includes positive electrode data that is an echo signal obtained when the slice gradient magnetic field is applied at the positive electrode in the main measurement, and An image reconstructing unit 721 that adds negative electrode data that is an echo signal obtained when the slice gradient magnetic field is applied at the negative electrode, and reconstructs an image using the polarity addition data after the addition,
- the pulse application amount calculation unit 712 applies the sign of each refocus pulse so as to reduce the side lobe signal of the excitation profile after adding the positive electrode data and the negative electrode data. To calculate the amount.
- the pre-processing unit 710 includes a slice gradient magnetic field waveform measurement unit 711 that measures a slice gradient magnetic field waveform of the pulse sequence, and the refocus pulse application amount calculation unit 712 includes the measured slice gradient magnetic field waveform. And the amount of each refocus pulse applied is calculated.
- the excitation profile of the positive electrode data and the negative electrode data does not have a phase that is inverted by 180 [deg] as theoretically due to the influence of distortion, offset, etc. of the slice gradient magnetic field pulse. Even if it exists, the influence by the slice gradient magnetic field applied extra can be excluded by application of a suitable refocusing pulse.
- the excitation profile of the polarity addition data can be a steep and good sidelobe and can be prevented from being mixed from signals other than the slice position designated in the reconstructed image. Therefore, a high-quality reconstructed image in which artifacts are suppressed can be obtained.
- the pre-processing unit 710 may further include an irradiation frequency calculation unit 713 that calculates the irradiation frequency of each half RF pulse as the correction value. At this time, the irradiation frequency calculation unit 713 calculates each irradiation frequency so as to eliminate the positional deviation between the two slice selective excitation positions, and the positional deviation is obtained from the measured slice gradient magnetic field waveform. It is calculated using the strength of the gradient magnetic field.
- the irradiation frequency of the half RF pulse is determined based on the measurement data of the actually applied slice gradient magnetic field waveform. For this reason, the displacement of the excitation position can be suppressed. Therefore, a steep excitation profile with fewer sidelobe signals can be obtained. As a result, a higher quality image can be obtained.
- the pre-processing unit 710 further includes a zero-order phase difference calculation unit 714 that calculates a zero-order phase difference, which is a zero-order term of the phase difference between the positive electrode data and the negative electrode data, as the correction value. Also good.
- the image reconstruction unit 721 corrects the phase difference between the positive electrode data and the negative electrode data using the zeroth-order phase difference before the addition.
- the 0th-order phase difference calculation unit 714 calculates the 0th-order phase difference using a difference between the slice gradient magnetic field waveform having the positive polarity and the slice gradient magnetic field waveform having the negative polarity.
- the phase difference between the positive electrode data and the negative electrode data is calculated based on the measurement data of the slice gradient magnetic field waveform actually applied. These data are corrected using the calculated phase difference. Therefore, it is possible to correct the phase difference with high accuracy and to obtain a better excitation profile. As a result, a higher quality image can be obtained.
- the case where the pre-processing is performed for each slice has been described as an example. This is because the output characteristics of the gradient magnetic field differ depending on the slice position, and the calculated values (irradiation frequency, applied amount, zero-order phase difference) vary depending on the position. However, it is not limited to this. For example, when there is no significant change in the output characteristics of the gradient magnetic field in accordance with the slice position, the above values may be calculated using only representative slice positions as processing targets. With this configuration, the processing can be speeded up.
- the side lobe signal can be effectively suppressed even in the multi-slice method. That is, in the multi-slice method, a plurality of slices are continuously excited in the TR, so that a side pulse signal cannot be suppressed by applying a saturation pulse adjacent to each slice plane. For this reason, when a saturation pulse is used, the saturation pulse is applied outside the entire imaging target region. Since signals in the range from the slice plane to the saturation pulse application position are not suppressed by the saturation pulse, signals from other than the designated slice position are mixed in the reconstructed image when a sidelobe signal is present. However, in the present embodiment, the shape of the excitation profile itself is improved and the sidelobe signal is reduced. For this reason, even if it is a multi-slice method, a sidelobe signal can fully be reduced and a high quality image can be obtained like other measurement.
- the pre-processing may be performed immediately before the actual measurement or may be performed at the time of installation of the apparatus.
- the obtained refocus pulse application amount, irradiation frequency, and zero-order phase difference are stored in the storage device 172 or the like in association with the slice gradient magnetic field from which the waveform is measured.
- the shift amount of the excitation position is calculated from the excitation profile of the positive electrode data and the negative electrode data, and the zero-order and first-order phase differences are calculated from the phase distribution of both data, and each correction value is obtained, and the pulse sequence And reflected in the reconstruction process.
- the MRI apparatus 100 of the present embodiment has basically the same configuration as that of the first embodiment.
- the pulse sequence used for imaging is also the UTE sequence 200 as in the first embodiment.
- the configuration of the pre-processing unit 710 is different.
- the present embodiment will be described focusing on the configuration different from the first embodiment.
- the pre-processing unit 710 of the present embodiment includes a refocus pulse application amount calculation unit 712, an irradiation frequency calculation unit 713, a zero-order phase difference calculation unit 714, and an excitation profile measurement unit 715.
- the arithmetic system 170 includes the preprocessing unit 710 and the main measurement unit 720, and the main measurement unit 720 includes the image reconstruction unit 721, as in the first embodiment.
- the pre-processing unit 710 of the first embodiment calculates each correction value based on the actually measured waveforms of the slice gradient magnetic fields 211 and 212.
- the pre-processing unit 710 of the present embodiment calculates a correction value from the excitation profile (intensity distribution and phase distribution) by the half RF pulse executed according to the set imaging parameter. That is, from the excitation profile, the shift amount of the excitation position and the zero-order and first-order phase differences between the positive electrode data and the negative electrode data that minimize the side lobe are calculated.
- the excitation profile measuring unit 715 measures the excitation profile for each slice and for each polarity of the slice gradient magnetic field.
- a pulse sequence (excitation profile measurement sequence) 500 shown in FIG. 14 is used.
- the excitation profile measurement sequence 500 includes the half RF pulses 501, 502, the positive slice gradient magnetic field 511 and the negative slice gradient magnetic field 512 applied together with the respective half RF pulses 501, 502, and the respective echo signals 541, 542. Read encoding gradient magnetic fields 531 and 532 applied in the slice direction.
- the excitation profile measurement unit 715 executes this excitation profile measurement sequence 500 using the imaging parameters for the main measurement. That is, the half RF pulses 501, 502, the positive electrode slice gradient magnetic field 511, and the negative electrode slice gradient magnetic field 512 are made to coincide with those used in the main measurement.
- the obtained echo signals 541 and 542 are each subjected to Fourier transform to obtain an excitation profile at the positive electrode and an excitation profile at the negative electrode.
- each obtained excitation profile is complex data, and has two pieces of information of phase distribution and intensity distribution.
- the intensity distribution Amp_positive (x) at the positive electrode and the intensity distribution Amp_negative () at the negative electrode are expressed by the equations (10) and (10), respectively. It is obtained in 11).
- x is a discrete point number representing a position in the slice direction
- real is a symbol representing a real part
- imgn is a symbol representing an imaginary part.
- the shift amount calculation unit 717 calculates the position shift Shift between the maximum value of the intensity distribution of the excitation profile 601 at the positive electrode and the maximum value of the intensity distribution of the excitation profile 602 at the negative electrode shown in the conceptual diagram of FIG. And calculated as the shift amount Shift of the excitation position. That is, the shift amount Shift of the excitation position is calculated according to, for example, Expression (12) to Expression (14) using the intensity distributions Amp_positive (x) and Amp_negative (x).
- Max () is a function that returns the maximum value in the specified data string
- MaxPositionPositive is the position of the maximum value of the positive excitation profile
- MaxPositionNagative is the value of the negative excitation profile Represents the position of the maximum value.
- the primary phase difference calculation unit 716 uses the respective excitation profiles Pre_positive () and Pre_negative () to calculate the primary term coefficient of the difference between the phase of the positive data and the phase of the negative data as the primary phase difference.
- phase difference Phase_complex (x) between the positive data and the negative data is calculated according to the following equation (15). Note that the phase difference Phase_complex (x) is complex data.
- Conjugate [] is a function representing complex conjugate processing
- Shift is a shift amount of the excitation position between the positive and negative electrodes calculated by Expression (12).
- phase value Phase_scalar (x) is calculated according to the following equation (16).
- the calculated phase value Phase_scalar (x) is scalar data.
- Phase [] is a function that returns the phase value of the complex data.
- the reason why the phase value is not calculated directly from Phase_complex (x) is to prevent the phase around the main value.
- the calculated phase value Phase_scalar (x) 611 changes as shown in FIG. That is, the phase changes 360 [deg] at the center 620 of the excitation range (which almost coincides with the position of the maximum value of the intensity distribution). This is because the positive electrode data and the negative electrode data have a change of 180 [deg] in opposite phases as shown in FIG.
- the primary phase difference is the slope of the calculated phase value Phase_scalar (x) 611. In order to obtain the primary phase difference (slope), it is necessary to exclude the phase change with the center 620 of the excitation range as a boundary and perform the phase unwrapping process.
- phase value Phase_scalar (x) the phase value Phase_scalar (x) after the phase unwrapping process is calculated.
- x represents a section other than the section 621 where the phase is changing
- PreviousePoint represents the position of the immediately preceding x.
- the primary phase difference calculation unit 716 determines an approximate primary line with respect to this phase distribution by the least square method, and calculates the inclination as the primary phase difference FirstOrderPhase. Specifically, it is calculated according to the following equation (19).
- N the number of data points used for the fitting process. Note that the fitting by the least square method is performed except for the section 621 where the phase changes.
- the refocus pulse application amount calculation unit 712 of this embodiment calculates the application amount of the refocus pulse of each slice gradient magnetic field 211, 212 as a correction value, as in the first embodiment.
- the surplus application amount is calculated from the slice gradient magnetic field waveform and the refocus pulse application amount is calculated, but in this embodiment, the refocus pulse application is performed using the first-order phase difference FirstOrderPhase. Calculate the amount.
- the refocus pulses 251 and 252 are pulses whose polarities are reversed, and in this case, both have the same area.
- the gradient of the primary phase difference of the excitation profile changes.
- the refocus area that is, the application amount of the refocus pulses 251 and 252 is calculated so as to create a phase gradient that cancels the calculated first order phase difference FirstOrderPhase.
- Adjust_Area_251 and Adjust_Area_252 [s ⁇ T / m] of the refocus pulses 251 and 252 are calculated according to the following equations (20) and (21), respectively.
- FirstOrderPhase is the primary phase difference [deg] calculated by the equation (19)
- Duration is the sampling time [s] of the echo signals 541 and 542 obtained in the excitation profile measurement sequence 500 of FIG.
- GcAmp is the intensity [T / m] of the read encode gradient magnetic fields 531 and 532.
- the irradiation frequency calculation unit 713 of the present embodiment calculates the irradiation frequencies of the half RF pulses 201 and 202 as correction values, as in the first embodiment.
- the position shift of each slice selective excitation position is determined from the slice gradient magnetic field intensity, and the irradiation frequency is calculated so as to eliminate it.
- the position deviation is determined and the irradiation frequency is calculated.
- the Larmor frequency at the specified slice position is usually set as the irradiation frequency. However, if the excitation position is shifted between the positive and negative data, it is necessary to change the irradiation frequency of the half RF pulses 201 and 202 by the shift amount so that the excitation positions of the positive and negative data match. is there.
- the irradiation frequency calculation unit 713 of this embodiment calculates an irradiation frequency that matches these excitation positions.
- the irradiation frequency is calculated for each of the half RF pulse 201 applied together with the positive electrode slice gradient magnetic field 211 and the half RF pulse 202 applied together with the negative electrode slice gradient magnetic field 212.
- the calculation is performed according to the following equations (22) and (23).
- Frequency_Positive is the irradiation frequency [Hz] of the half RF pulse when the slice gradient magnetic field is positive
- Frequency_Nagative is the irradiation frequency [Hz] of the half RF pulse when the slice gradient magnetic field is negative
- ⁇ is the magnetic rotation ratio [Hz / T]
- Gs is the slice gradient magnetic field strength [T / m]
- Offcenter is the distance [m] from the magnetic field center to the specified slice position
- Shift is the positive and negative data calculated by the above equation (12).
- GcBase is the static magnetic field strength [T].
- the 0th-order phase difference calculation unit 714 of the present embodiment calculates the 0th-order phase difference between the positive data and the negative data as a correction value.
- the zero-order phase difference is calculated from the slice gradient magnetic field waveform, but in this embodiment, the phase value Phase_unwraped (xx) after phase unwrapping obtained from the excitation profile at the positive electrode and the excitation profile at the negative electrode is obtained. ) Is used to calculate the zeroth-order phase difference according to the following equation (24).
- x excludes the section 1501 where the phase changes.
- the value calculated from Equation (24) is a value obtained by subtracting from 180 [deg] the phase difference obtained by removing the primary phase gradient from the phase difference between the positive electrode data and the negative electrode data.
- the positive and negative data have a phase difference of 180 [deg]
- the side lobe signals cancel each other. Therefore, the difference from 180 [deg] of the phase difference between the two data is calculated as the 0th order phase difference.
- the preprocessing unit 710 performs preprocessing for calculating a correction value for each slice.
- the excitation profile is measured over all slices, and then a correction value is calculated for each slice.
- the excitation profile measurement unit 715 executes the excitation profile measurement sequence 500 for each slice using the imaging parameters at the time of this measurement, and the excitation profile Pre_positive () when the slice gradient magnetic field is positive and the slice gradient magnetic field is negative Are respectively acquired (steps S2101 to S2104).
- the pre-processing unit 710 repeats the processing from step S2106 to step S2110 through repetitive processing (step S2105, step S2211).
- the number of repetitions is the number of slices (N in this case) specified as the imaging condition for the main measurement.
- i represents the slice number to be processed during the repeated processing.
- the shift amount calculation unit 717 calculates the shift amount Shift of the excitation position at the i-th slice position from both excitation profiles at the i-th slice position using the above formulas (12) to (14). (Step S2106).
- the primary phase difference calculation unit calculates the primary phase difference FirstOrderPhase at the i-th slice position from both excitation profiles at the i-th slice position by the above equations (15) to (19). (Step S2107).
- the refocus pulse application amount calculation unit 712 uses the primary phase difference FirstOrderPhase of the i-th slice position, and applies the application amount of the refocus pulses 251 and 252 to each slice gradient magnetic field at the i-th slice position. Calculations are performed respectively using Equation (20) and Equation (21) (Step S2108).
- the irradiation frequency calculation unit 713 uses the calculated shift amount Shift, and the irradiation frequency of each half RF pulse 201, 202 at the i-th slice position by the above formula (22) and formula (23), Each is calculated (step S2109).
- the 0th-order phase determination unit uses the first-order phase difference FirstOrderPhase at the i-th slice position, and calculates the 0th-order phase difference between the positive electrode data and the negative electrode data at the i-th slice position by the above formula (24 ) (Step S2110).
- the pre-processing unit 710 of the present embodiment performs pre-processing, and calculates correction values for the irradiation frequencies of the half RF pulses 201 and 202, the application amounts of the refocus pulses 251 and 252 and the zero-order phase difference, respectively. .
- any of the calculation of the irradiation frequency, the calculation of the refocus pulse application amount, and the calculation of the zero-order phase may be performed first.
- FIG. 18 (a) is an intensity distribution 801 of the excitation profile of each of the positive and negative data obtained by executing the excitation profile measurement sequence 500 using the irradiation frequency and refocus pulse application amount set by the imaging parameters. 802.
- FIG. 18 (b) shows the polarity addition data obtained by adding the positive polarity data and the negative polarity data obtained by executing the excitation profile measurement sequence 500 using the irradiation frequency and the refocus pulse application amount set by the imaging parameters as they are. It is an intensity distribution 803 of the excitation profile.
- FIG. 18 (c) shows an intensity distribution 813 of the excitation profile of the polarity addition data obtained by changing the irradiation frequency to the correction value and executing the excitation profile measurement sequence 500.
- FIG. 18D shows an excitation profile intensity distribution 823 of polarity addition data obtained by changing the application amount of the refocus pulse to a correction value and executing the excitation profile measurement sequence 500.
- FIG. 18 (e) shows positive and negative data obtained by executing the excitation profile measurement sequence 500 using the irradiation frequency and refocus pulse application amount set by the imaging parameters, using the zeroth-order phase difference. It is an intensity distribution 833 of the excitation profile of the polarity addition data obtained by addition after correction.
- FIG. 18 (e) shows an intensity distribution 813 of the excitation profile of the polarity addition data obtained by changing the irradiation frequency to the correction value and executing the excitation profile measurement sequence 500.
- FIG. 18D shows an excitation profile intensity distribution 823 of polarity addition data obtained by changing the application
- FIG. 18 (f) shows an intensity distribution 843 of the excitation profile of the polarity addition data obtained by changing the irradiation frequency and the refocus pulse application amount to the correction values and executing the excitation profile measurement sequence 500.
- FIG. 18 (g) shows that the irradiation frequency and the refocus pulse application amount are changed to correction values, the excitation profile measurement sequence 500 is executed, and positive electrode data and negative electrode data are added after correction using the zeroth-order phase difference. It is an intensity distribution 853 of the excitation profile of the obtained polarity addition data.
- a sharp excitation profile can be obtained and specified by adjusting the shift amount of the excitation position (irradiation frequency), the primary phase difference (refocus pulse application amount), and the zeroth phase difference. It is possible to suppress mixing of signals from other than the slice position. It can be seen that adjustment of the primary phase difference (adjustment of the refocus pulse application amount) is particularly effective.
- FIGS. 18 (a) to 18 (e) show the excitation profiles measured by pre-processing, but the same can be said for this measurement. Images obtained by reconstructing the data acquired in this measurement process are shown in FIGS. 19 (a) and 19 (b).
- the object to be imaged is a conical nickel chloride aqueous solution phantom, and the imaging section is set so that the diameter of the circle changes in the slice direction.
- An image 861 shown in FIG. 19 (a) is a result image when this measurement is performed without using the three correction values (irradiation frequency, refocus pulse application amount, and zeroth-order phase difference) obtained by the pre-processing.
- the image 862 is a result image obtained by reflecting each correction value determined by the above method.
- a profile 871 shown in FIG. 19 (c) is a profile of a position indicated by a dotted line on the image 861
- a profile 872 shown in FIG. 19 (d) is a profile of a position indicated by a dotted line on the image 862. .
- each intensity distribution Amp_positive (x), Amp_negative (x), and a value that maximizes the cross-correlation value may be obtained as the shift amount Shift.
- the shift amount Shift may be obtained from the gradient of the phase difference in the space obtained by Fourier transforming each intensity distribution Amp_positive (x) and Amp_negative (x).
- the shift amount calculation unit 717 and the irradiation frequency calculation unit 713 may not be provided.
- the value of the variable Shift in the equation (15) for calculating the phase difference Phase_complex (x) is 0.
- the irradiation frequency used in the main measurement is specified by the imaging parameter.
- the 0th-order phase difference calculation unit 714 may not be provided. If not implemented, 0 [deg] may be set as the phase difference.
- the measurement system includes the static magnetic field generation system 120, the gradient magnetic field generation system 130, the high-frequency magnetic field generation system 150, and the high-frequency magnetic field detection system 160, and the measurement system according to the pulse sequence.
- a magnetic resonance imaging apparatus comprising: an operation system 170 that controls the operation of the magnetic resonance signal to measure a nuclear magnetic resonance signal and performs an operation using data obtained from the nuclear magnetic resonance signal.
- This is an ultra-short echo time sequence in which the slice gradient magnetic field applied together with the RF pulse is inverted between the positive and negative electrodes to perform two slice selective excitations to obtain echo signals, respectively.
- a pre-processing unit 710 that calculates a correction value used for the calculation, and the correction value calculated by the pre-processing unit 710 is set in the pulse sequence
- a main measurement unit 720 that controls the measurement system according to a pulse sequence to perform main measurement and reconstructs an image, and the pre-processing unit 710 determines an application amount of a refocus pulse of each slice gradient magnetic field.
- Refocusing pulse application amount calculation unit 712 for calculating each as the correction value and the main measurement unit 720 includes positive electrode data that is an echo signal obtained when the slice gradient magnetic field is applied at the positive electrode in the main measurement, and An image reconstruction unit 721 that adds the negative electrode data, which is an echo signal obtained when the slice gradient magnetic field is applied at the negative electrode, and reconstructs an image using the polarity addition data after the addition,
- the focus pulse application amount calculation unit 712 applies the sign of each refocus pulse so as to reduce the side lobe signal of the excitation profile after adding the positive electrode data and the negative electrode data. To calculate the amount.
- the pre-processing unit uses an excitation profile measurement unit 715 that measures the excitation profile of each of the positive electrode data and the negative electrode data, and uses each of the excitation profiles, and calculates the coefficient of the primary term of the phase difference as a primary phase difference
- the refocus pulse application amount calculation unit 712 determines each refocus pulse application amount using the primary phase difference.
- the phase difference between the positive electrode data and the negative electrode data is calculated, and the primary phase difference is corrected by adjusting the refocus pulse application amount of the slice gradient magnetic field pulse.
- the side lobe signal of the excitation profile can be effectively suppressed, and the excitation profile of the polarity addition data can be good with a steep and few side lobe, from other than the slice position specified in the reconstructed image. Can be prevented from being mixed. Therefore, a high-quality reconstructed image in which artifacts are suppressed can be obtained.
- the pre-processing unit 710 includes an irradiation frequency calculation unit 713 that calculates the irradiation frequency of each half RF pulse as the correction value, and a shift amount calculation unit that calculates the shift amount of the excitation position between the excitation profiles. 717 may be further included.
- the irradiation frequency calculation unit 713 calculates the respective irradiation frequencies so as to eliminate the positional deviation between the two slice selective excitation positions, and the positional deviation is calculated using the shift amount.
- the excitation position shift amount between the positive electrode data and the negative electrode data is calculated by measuring the excitation profile in the pre-processing, the irradiation frequency of the half RF pulses 201 and 202 is adjusted, and the deviation of the excitation position is calculated. Correct.
- the pre-processing unit 710 further includes a zero-order phase difference calculation unit 714 that calculates a zero-order phase difference, which is a zero-order term of the phase difference between the positive electrode data and the negative electrode data, as the correction value. Also good.
- the 0th-order phase difference calculation unit 714 calculates the 0th-order phase difference using each excitation profile.
- the image reconstruction unit 721 corrects the phase difference between the positive electrode data and the negative electrode data before the addition using the zeroth-order phase difference.
- the 0th-order phase difference is corrected by adding the phase during the addition process after the acquisition of the main measurement data.
- a steep excitation profile is obtained, and signals from other than the designated slice position are not mixed in the reconstructed image, and a reconstructed image in which artifacts are suppressed is obtained.
- the pre-processing may be performed immediately before the main measurement or may be performed at the time of installation of the apparatus.
- pre-processing is executed under the conditions of combinations of all slice positions and slice thicknesses that can be designated in the main measurement processing. Or you may perform a pre-processing only by typical conditions. In either case, the obtained excitation position shift amount and first-order phase difference, or refocus pulse application amount, irradiation frequency, and zero-order phase difference are stored in the storage device 172 or the like in association with the calculation conditions. Keep it.
- the pre-processing is divided into the excitation profile measurement processing and the correction value calculation processing using the excitation profile measurement processing, and each is repeated by the number of slices.
- This is because it is considered that the excitation profile is measured under the same measurement conditions as the main measurement. That is, when excitation of a plurality of slices is performed within a repetition time (TR) by a multi-slice method or the like, it may not be possible to obtain a time for calculating a correction value. In this way, a more accurate correction value can be obtained by performing slice excitation under the same conditions as in the main measurement process.
- TR repetition time
- each correction value in steps S2106 to S2110 can be secured after the excitation of each slice and the measurement of the excitation profile, it is not necessary to divide the repetition process into two. For each slice, the measurement of the excitation profile and the calculation of the correction value may be performed as a series of processes.
- the MRI apparatus 100 of the present embodiment has basically the same configuration as that of the first embodiment. However, since the calculation methods of the primary phase difference and the zeroth phase difference are different, the configuration of the preprocessing unit 710 of the arithmetic system 170 is different.
- the pre-processing unit 710 of the present embodiment includes an excitation profile measurement unit 715, a shift amount calculation unit 717, a refocus pulse application amount calculation unit 712, an irradiation frequency calculation unit 713, a phase difference, And an optimum value search unit 718.
- the arithmetic system 170 includes the pre-processing unit 710 and the main measurement unit 720, and the main measurement unit 720 includes the image reconstruction unit 721, as in the second embodiment.
- the processing of the excitation profile measurement unit 715, the shift amount calculation unit 717, and the irradiation frequency calculation unit 713 of the present embodiment is the same as that of the second embodiment.
- the irradiation frequency calculation in the pre-processing flow by the pre-processing unit 710 of the present embodiment is basically the same as in the second embodiment. That is, as shown in FIG. 17, the excitation profile is measured for each slice position, and using this, the shift amount of the excitation position is calculated, and the irradiation frequency is calculated.
- the phase difference optimal value search unit 718 of the present embodiment changes the primary phase difference and the zeroth phase difference from a predetermined initial value according to a predetermined rule, and sets a value (optimum value) that minimizes the evaluation value. Explore. Then, the obtained optimum values are defined as a first-order phase difference and a zero-order phase difference, respectively. At this time, the signal value of the side lobe obtained from each excitation profile is used as the evaluation value.
- the refocus pulse application amount calculation unit 712 of the present embodiment uses the primary phase difference obtained as the optimum value by the phase difference optimal value search unit 718, and sets the refocus pulse application amount as in the second embodiment. Calculate according to the procedure.
- the image reconstruction unit 721 corrects the polarity addition data using the zeroth-order phase difference obtained as the optimum value by the phase difference optimum value search unit 718.
- the flow of the preprocessing by the preprocessing unit 710 of this embodiment is basically the same as the flow of the preprocessing of the second embodiment shown in FIG.
- the optimal value search process for the primary phase difference and the zeroth phase difference by the phase difference optimal value search unit 718 is performed.
- the primary phase difference and the zeroth phase difference are calculated.
- the 0th-order phase difference calculation process in step S2110 is not performed.
- the main measurement process of the present embodiment is the same as that of the first embodiment.
- the phase difference optimum value search unit 718 sets the initial values of the predetermined primary phase difference and the zeroth phase difference as the primary phase difference optimum value candidate and the zeroth order phase difference optimum value candidate, respectively (step S3101).
- 0 [deg] is set as the initial value.
- similar to an optimal value is known beforehand from the characteristic of an apparatus, you may set the value.
- the optimum phase difference search unit 718 searches for the primary phase difference that minimizes the signal amount of the side lobe (step S3102), and updates the optimal value candidate for the primary phase difference (step S3103).
- Sidelobe signal amount (hereinafter referred to as sidelobe amount) SideLoveValue is defined by the following equation (25), for example.
- Amp_composed () is the pre-excitation excitation profile Pre_Positive () and negative-excitation excitation profile Pre_Negative () obtained by pre-processing, and the primary phase difference and zero-order phase difference at this time point, respectively. This is the data added in the set state, and is obtained by the following equations (26) to (30). Note that Pre_Negative () in the following equation is treated as being shifted by the shift amount calculated by the shift amount calculation unit 717.
- x is a discrete point number representing a position in the slice direction
- real is a symbol representing a real part
- imgn is a symbol representing an imaginary part
- ZerothOrderPhase is a zero-order phase difference
- FirstOrderPhase is a first-order phase difference.
- MainLobeRange in equation (25) is the range of the main lobe, and is defined by the following equation (31), for example.
- Offcenter is the distance [m] from the magnetic field center to the designated slice position
- Thickness is the designated slice thickness [m].
- the primary phase difference is 0.1 [deg] within a sufficiently wide range, for example, in the range of ⁇ 3600 [deg] to 3600 [deg].
- the amount of side lobe is calculated, and the primary phase difference that minimizes the side lobe amount is determined as the optimum value of the primary phase difference.
- the phase difference optimal value search unit 718 searches for the 0th-order phase difference that minimizes the side lobe amount (step S3104), and The optimum value candidate is updated (step S3105).
- the search method is the same as the search for the primary phase difference. However, since it is the 0th order phase, the search range is set to ⁇ 180 [deg] to 180 [deg]. This range is changed in increments of 0.1 [deg] to calculate the side lobe amount, and the zeroth-order phase difference that minimizes the side lobe amount is determined as the optimum value candidate.
- the phase difference optimum value search unit 718 stores the side lobe amount that is the calculated evaluation value in association with the number of times of calculation of the zeroth phase difference (step S3106).
- the phase difference optimum value search unit 718 determines whether or not the change in the side lobe amount that is the evaluation value has converged (step S3107).
- the convergence of the change in the side lobe amount is defined by the following equation (32), for example.
- SideLobeValue (n) represents the side lobe amount recorded for the nth time.
- Equation (32) represents the convergence condition when the change in the side lobe amount is less than 0.1 [%] while the search process for the first-order phase difference and the zero-order phase difference is repeated.
- step S3107 phase difference optimum value search section 718 needs to be repeated at least twice in order to compare with the side lobe amount recorded in the previous search.
- the phase difference optimum value search unit 718 ends the optimum value search process when the expression (32) is satisfied. Then, the optimum value candidates for the primary phase difference and the 0th order phase difference at that time are set as the primary phase difference and the 0th order phase difference.
- the measurement system includes the static magnetic field generation system 120, the gradient magnetic field generation system 130, the high-frequency magnetic field generation system 150, and the high-frequency magnetic field detection system 160, and the measurement system according to the pulse sequence.
- a magnetic resonance imaging apparatus comprising: an operation system 170 that controls the operation of the magnetic resonance signal to measure a nuclear magnetic resonance signal and performs an operation using data obtained from the nuclear magnetic resonance signal.
- This is an ultra-short echo time sequence in which the slice gradient magnetic field applied together with the RF pulse is inverted between the positive and negative electrodes to perform two slice selective excitations to obtain echo signals, respectively.
- a pre-processing unit 710 that calculates a correction value used for the calculation, and the correction value calculated by the pre-processing unit 710 is set in the pulse sequence
- a main measurement unit 720 that controls the measurement system according to a pulse sequence to perform main measurement and reconstructs an image, and the pre-processing unit 710 determines an application amount of a refocus pulse of each slice gradient magnetic field.
- Refocusing pulse application amount calculation unit 712 for calculating each as the correction value includes positive electrode data that is an echo signal obtained when the slice gradient magnetic field is applied at the positive electrode in the main measurement, and An image reconstruction unit 721 that adds the negative electrode data, which is an echo signal obtained when the slice gradient magnetic field is applied at the negative electrode, and reconstructs an image using the polarity addition data after the addition.
- the focus pulse application amount calculation unit 712 applies the sign of each refocus pulse so as to reduce the side lobe signal of the excitation profile after adding the positive electrode data and the negative electrode data. To calculate the amount.
- the pre-processing unit 710 includes an excitation profile measurement unit 715 that measures the excitation profile of each of the positive electrode data and the negative electrode data, and a coefficient of a primary term of a phase difference between the positive electrode data and the negative electrode data.
- a certain first-order phase difference and a zero-order phase difference that is a zero-order term of the phase difference are changed from a predetermined initial value according to a predetermined rule, and a value that minimizes an evaluation value is searched for.
- a phase difference optimum value search unit 718 that determines an optimum value of the next phase difference and the zeroth order phase difference, and the evaluation value is a signal amount of a side lobe obtained from the respective excitation profiles
- the refocus pulse application amount calculation unit 712 determines the refocus pulse application amount using the primary phase difference
- the image reconstruction unit 721 determines whether the positive data and the negative data before the addition.
- the phase difference is corrected using the optimum value of the zeroth-order phase difference.
- the phase difference optimum value search unit 718 fixes the zero-order phase difference to the optimum value of the zero-order phase difference, changes the primary phase difference according to a predetermined rule, and calculates the evaluation value.
- the primary phase difference to be minimized is determined as the optimal value of the primary phase difference, the primary phase difference is fixed to the optimal value of the primary phase difference, and the zero-order phase difference is changed according to a predetermined rule.
- the zeroth-order and first-order phase differences are searched based on the side lobe amount.
- the method of the present embodiment has the smallest side lobe signal amount even when it is difficult to fit a linear line to the phase distribution, that is, when the phase distribution draws a high-order curve.
- a zero-order phase difference and a first-order phase difference can be calculated. Therefore, irrespective of the static magnetic field uniformity of the apparatus, the excitation profile can be made good with high accuracy, and a high-quality image can be obtained.
- the side lobe signal amount defined by Expression (25) is used as the evaluation value.
- Equation (25) is intended to calculate the amount of signal in a range other than the main lobe in the excitation profile. Therefore, as long as the signal amount other than the main lobe can be grasped, an evaluation expression (evaluation value) other than Expression (25) may be used.
- the evaluation formula may be a form in which the side lobe amount is normalized by the main lobe signal amount.
- the evaluation formula may be such that the signal intensity of the side lobe is weighted in proportion to the distance from the designated slice position, and the side lobe amount is calculated.
- each is changed by a predetermined fixed change amount, but is not limited thereto.
- the search may be performed using a search algorithm typified by the golden section method, etc., independently for each of the first-order phase difference and the zero-order phase difference.
- the first-order phase difference and the zero-order phase difference may be combined and searched using a multidimensional search algorithm typified by the downhill simplex method or the multidimensional conjugate gradient method.
- the shift amount calculation unit 717 and the irradiation frequency calculation unit 713 may not be provided.
- the irradiation frequency used in the main measurement is specified by the imaging parameter.
- the phase difference optimum value search unit 718 may search for the optimum value only for the primary phase difference.
- the phase difference is handled as a fixed value (for example, 0 [deg]).
- the pre-processing may be performed immediately before the main measurement or may be performed at the time of installation of the apparatus.
- pre-processing is executed under the conditions of combinations of all slice positions and slice thicknesses that can be designated in the main measurement processing. Or you may perform a pre-processing only by typical conditions. In either case, the obtained result is stored in the storage device 172 or the like in association with the calculation condition.
- the present embodiment is characterized in that the calculation accuracy of the excitation position shift amount and the primary phase difference is improved by performing the pre-processing a plurality of times.
- the MRI apparatus 100 of this embodiment basically has the same configuration as that of the first embodiment.
- the configuration of the arithmetic system 170 is basically the same as that of the second embodiment.
- the pre-processing unit 710 further includes a convergence determination unit 719 in order to repeatedly calculate the primary phase difference and the shift amount and improve the calculation accuracy. . Also, the processing itself of the pre-processing unit 710 is different.
- the convergence determination unit 719 of the present embodiment satisfies a predetermined convergence condition each time the primary phase difference calculation unit 716 and the shift amount calculation unit 717 calculate the primary phase difference and the shift amount, respectively. It is determined whether or not.
- the pre-processing unit 710 of this embodiment proceeds with processing according to the determination result. Specifically, if the determination result is negative, the refocus pulse application amount calculation unit 712 calculates the refocus pulse application amount using the calculated primary phase difference, and the irradiation frequency calculation unit 713 sets the irradiation frequency. Using these, the excitation profile measurement unit 715 is caused to execute the excitation profile measurement sequence 500 to cause the excitation profile to be measured again. On the other hand, if the determination result is satisfactory, the 0th-order phase difference calculation unit is caused to calculate the 0th-order phase difference from the excitation profile obtained by calculating the 1st-order difference.
- the pre-processing unit 710 of the present embodiment sets the irradiation frequency set by the imaging parameters and the application amount of the refocus pulse (Step S4101). Then, the excitation profile measurement unit 715 executes the excitation profile measurement sequence 500, and measures the excitation profile at the positive electrode and the excitation profile at the negative electrode, respectively, using the same method as in the second embodiment (step S4102).
- the shift amount calculation unit 717 calculates the shift amount Shift of the excitation position according to the equations (12) to (14) by the same method as in the second embodiment (step S4103).
- the primary phase difference calculation unit calculates the primary phase difference FirstOrderPhase according to the equations (15) to (19) using the same method as in the second embodiment (step S4104).
- the preprocessing unit 710 stores the calculated shift amount shift and primary phase difference FirstOrderPhase in the storage device 172 in association with the number of calculations (step S4105).
- the convergence determination unit 719 satisfies the convergence condition using the currently calculated shift amount shift and primary phase difference FirstOrderPhase and the previously calculated excitation position shift amount shift and primary phase difference FirstOrderPhase. Whether or not each value has converged (step S4106).
- Shift (n) is the shift amount recorded at the nth time
- FirstOrderPhase (n) is the primary phase recorded at the nth time.
- Expressions (33) and (34) represent convergence conditions when the respective change rates become less than 0.1 [%] while the calculation of the shift amount and the primary phase is repeated.
- the convergence determination unit 719 outputs “No” as the determination result.
- the pre-processing unit 710 applies the refocus pulse application from the primary phase difference FirstOrderPhase to the refocus pulse application amount calculation unit 712 using the equations (20) and (21) as in the second embodiment.
- the amount is calculated (step S4107).
- the irradiation frequency calculation unit 713 uses the expressions (22) and (23) to calculate the irradiation frequency from the calculated shift amount Shift (step S4108). Note that either the calculation of the irradiation frequency or the calculation of the refocus pulse application amount may be performed first.
- the pre-processing unit 710 sets the calculated irradiation frequency and refocus pulse application amount in the excitation profile measurement sequence 500, returns to step S4102, and repeats the process.
- step S4106 the convergence determination unit 719 outputs a determination result that the convergence condition is satisfied.
- the preprocessing unit 710 terminates the iterative process, and uses the first-order phase difference FirstOrderPhase at that time for the 0th-order phase difference calculation unit 714, in the same manner as in the second embodiment, using the equation (24 ) To calculate the zero-order phase difference (step S4109).
- the measurement system includes the static magnetic field generation system 120, the gradient magnetic field generation system 130, the high-frequency magnetic field generation system 150, and the high-frequency magnetic field detection system 160, and the measurement system according to the pulse sequence.
- a magnetic resonance imaging apparatus comprising: an operation system 170 that controls the operation of the magnetic resonance signal to measure a nuclear magnetic resonance signal and performs an operation using data obtained from the nuclear magnetic resonance signal.
- This is an ultra-short echo time sequence in which the slice gradient magnetic field applied together with the RF pulse is inverted between the positive and negative electrodes to perform two slice selective excitations to obtain echo signals, respectively.
- a pre-processing unit 710 that calculates a correction value used for the calculation, and the correction value calculated by the pre-processing unit 710 is set in the pulse sequence
- a main measurement unit 720 that controls the measurement system according to a pulse sequence to perform main measurement and reconstructs an image, and the pre-processing unit 710 determines an application amount of a refocus pulse of each slice gradient magnetic field.
- Refocusing pulse application amount calculation unit 712 for calculating each as the correction value includes positive electrode data that is an echo signal obtained when the slice gradient magnetic field is applied at the positive electrode in the main measurement, and An image reconstruction unit 721 that adds the negative electrode data, which is an echo signal obtained when the slice gradient magnetic field is applied at the negative electrode, and reconstructs an image using the polarity addition data after the addition.
- the focus pulse application amount calculation unit 712 applies the sign of each refocus pulse so as to reduce the side lobe signal of the excitation profile after adding the positive electrode data and the negative electrode data. To calculate the amount.
- the pre-processing unit 710 uses the excitation profile measurement unit 715 that measures the excitation profile of each of the positive electrode data and the negative electrode data, and uses each of the excitation profiles, and uses the first-order coefficient of the phase difference as the first order.
- a primary phase difference calculation unit 716 that calculates the phase difference, and the refocus pulse application amount calculation unit 712 determines the refocus pulse application amount using the primary phase difference.
- the pre-processing unit 710 includes an irradiation frequency calculation unit 713 that calculates the irradiation frequency of each half RF pulse as the correction value, and a shift amount calculation unit that calculates the shift amount of the excitation position between the excitation profiles. 717 may be further included.
- the irradiation frequency calculation unit 713 calculates the respective irradiation frequencies so as to eliminate the positional deviation between the two slice selective excitation positions, and the positional deviation is calculated using the shift amount.
- the pre-processing unit 710 further includes a zero-order phase difference calculation unit 714 that calculates a zero-order phase difference, which is a zero-order term of the phase difference between the positive electrode data and the negative electrode data, as the correction value. Also good.
- the 0th-order phase difference calculation unit 714 calculates the 0th-order phase difference using each excitation profile.
- the image reconstruction unit 721 corrects the phase difference between the positive electrode data and the negative electrode data before the addition using the zeroth-order phase difference.
- the pre-processing unit 710 calculates the primary phase difference and the shift amount each time the primary phase difference calculation unit and the shift amount calculation unit calculate the primary phase difference and the shift amount, respectively.
- the calculation unit calculates the first-order phase difference and the shift amount calculation unit calculates the shift amount, and the determination result satisfies the convergence condition, the zero-order The phase difference calculation unit 714, to calculate the zero-order retardation latest from said respective excitation profile.
- the optimum irradiation frequency and refocus pulse application amount are determined while feeding back the calculation result to the pulse sequence. For example, when the pulse sequence is changed, the shift amount and the primary phase gradient may not be completely cancelled. However, according to the present embodiment, since iterative processing is performed until a predetermined convergence condition is satisfied, a more appropriate shift amount and primary phase can be calculated. As a result, a more appropriate refocus pulse application amount and irradiation frequency can be obtained and reflected in the pulse sequence.
- the calculation of the zeroth phase difference is not included in the iterative process. This is because the reconstruction process uses the 0th order phase and does not involve a change in the pulse sequence. Therefore, according to the present embodiment, after determining an optimal pulse sequence, a zero-order phase difference can be obtained and reflected in image reconstruction. Thereby, according to this embodiment, the optimal irradiation frequency, refocus pulse application amount, and zero-order phase difference can be obtained efficiently.
- the convergence condition is defined in advance, but the determination of convergence is not limited to this.
- the primary phase difference and the shift amount may be determined by repeating a certain number of times without setting the convergence condition, and the irradiation frequency and the refocus pulse application amount may be calculated.
- the shift amount calculation unit 717 and the irradiation frequency calculation unit 713 may not be provided.
- the value of the variable Shift in the equation (15) for calculating the phase difference Phase_complex (x) is 0.
- the irradiation frequency used in the main measurement is specified by the imaging parameter.
- the 0th-order phase difference calculation unit 713 may not be provided. If not implemented, the phase difference may be set to 0 [deg].
- the case where the primary phase difference and the zeroth phase difference are calculated using the method of the second embodiment is described as an example, but the present invention is not limited to this.
- the first-order phase difference and the zero-order phase difference may be calculated using the method of the third embodiment.
- the first-order phase difference is fixed to 0 [deg] and the 0th-order phase difference is searched.
- the pre-processing may be performed immediately before the main measurement or may be performed at the time of installation of the apparatus.
- pre-processing is executed under the conditions of combinations of all slice positions and slice thicknesses that can be designated in the main measurement processing. Or you may perform a pre-processing only by typical conditions. In either case, the obtained result is stored in the storage device 172 or the like in association with the calculation condition.
- the optimum irradiation frequency of the RF pulse and the application amount of the refocusing pulse of the slice gradient magnetic field are set, and the positive electrode data and A good excitation profile can be obtained by adding a zero-order phase difference when complex addition of negative electrode data is performed.
- a signal from other than the designated slice position is not mixed in the reconstructed image, and a reconstructed image in which artifacts are suppressed can be obtained. This is particularly effective in the case of measurement using a multi-slice method in which the side lobe signal of the excitation profile cannot be suppressed by the saturation pulse.
- 100 MRI apparatus 101 subject, 120 static magnetic field generation system, 130 gradient magnetic field generation system, 131 gradient magnetic field coil, 132 gradient magnetic field power supply, 140 sequencer, 150 high frequency magnetic field generation system, 151 transmission coil, 152 synthesizer, 153 modulator, 154 high frequency amplifier, 160 high frequency magnetic field detection system, 161 receiver coil, 162 signal amplifier, 163 quadrature detector, 164 D converter, 170 arithmetic system, 171 CPU, 172 storage device, 173 external storage device, 174 display device, 175 Input device, 200 UTE sequence, 201 half RF pulse, 202 half RF pulse, 211 slice gradient magnetic field, 211 positive slice gradient magnetic field, 212 slice gradient magnetic field, 212 negative slice gradient magnetic field, 221 phase encode gradient magnetic field, 222 phase encode gradient magnetic field , 231 Read encode gradient magnetic field, 232 Read encode read gradient magnetic field, 241 Echo signal 251 refocus pulse, 252 refocus pulse, 301 excitation profile, 302 excitation profile, 303 excitation profile
Landscapes
- Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
- Life Sciences & Earth Sciences (AREA)
- High Energy & Nuclear Physics (AREA)
- General Health & Medical Sciences (AREA)
- Radiology & Medical Imaging (AREA)
- General Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- Heart & Thoracic Surgery (AREA)
- Medical Informatics (AREA)
- Molecular Biology (AREA)
- Surgery (AREA)
- Animal Behavior & Ethology (AREA)
- Biophysics (AREA)
- Public Health (AREA)
- Veterinary Medicine (AREA)
- Biomedical Technology (AREA)
- Pathology (AREA)
- Signal Processing (AREA)
- Magnetic Resonance Imaging Apparatus (AREA)
Abstract
Description
本発明を適用する第一の実施形態について図面を用いて説明する。なお、発明の実施形態を説明するための全図において、同一機能を有するものは同一符号を付け、その繰り返しの説明は省略する。
式(5)において、Waveform_positive(x)とWaveform_negative(y)とを逆にし、負極データに対する正極データの位相のずれを算出してもよい。
次に、本発明を適用する第二の実施形態を説明する。本実施形態は、正極データと負極データの励起プロファイルから励起位置のシフト量を算出するとともに、両データの位相分布から0次と1次の位相差を算出し、各補正値を得、パルスシーケンス及び再構成処理に反映させる。
なお、演算系170が、事前処理部710と本計測部720とを備えること、および、本計測部720が、画像再構成部721を備えることは、第一の実施形態と同様である。
1次位相差算出部716は、この位相分布に対して最小二乗法により近似1次直線を決定し、その傾きを1次位相差FirstOrderPhaseとして算出する。具体的には、次の式(19)に従って算出する。
従って、アーチファクトが抑制された高い品質の再構成画像を得ることができる。
次に、本発明を適用する第三の実施形態について説明する。本実施形態は、励起プロファイルのサイドローブの信号量を基準として最適な1次と0次の位相差を探索して算出することを特徴とする。
次に、本発明を適用する第四の実施形態を説明する。本実施形態は、事前処理を複数回行うことで、励起位置のシフト量、1次位相差の算出精度を向上させることを特徴とする。
また、事前処理部710の処理自体も異なる。
特に、飽和パルスによって励起プロファイルのサイドローブ信号を抑制することができないマルチスライス法を用いた計測の場合に有効である。
Claims (20)
- 静磁場発生系と、傾斜磁場発生系、高周波磁場発生系および高周波磁場検出系を備える計測系と、パルスシーケンスに従って、前記計測系の動作を制御して核磁気共鳴信号を計測するとともに前記核磁気共鳴信号から得たデータを用いて演算を行う演算系と、を備える磁気共鳴イメージング装置であって、
前記パルスシーケンスは、ハーフRFパルスとともに印加するスライス傾斜磁場の極性を正極と負極との間で反転させて2回のスライス選択励起を行い、それぞれエコー信号を得る超短エコー時間シーケンスであり、
前記演算系は、
前記計測および前記演算に用いる補正値を算出する事前処理部と、
前記事前処理部で算出した補正値を前記パルスシーケンスに設定し、設定後の当該パルスシーケンスに従って前記計測系を制御して本計測を行い、画像を再構成する本計測部と、を備え、
前記事前処理部は、前記各スライス傾斜磁場のリフォーカスパルスの印加量をそれぞれ前記補正値として算出するリフォーカスパルス印加量算出部を備え、
前記本計測部は、前記本計測において、前記スライス傾斜磁場を正極で印加した際に得たエコー信号である正極データと、前記スライス傾斜磁場を負極で印加した際に得たエコー信号である負極データとを加算し、加算後の極性加算データを用いて画像を再構成する画像再構成部を備え、
前記リフォーカスパルス印加量算出部は、前記正極データと前記負極データとを加算した後の励起プロファイルのサイドローブ信号を低減させるよう前記各リフォーカスパルスの印加量を算出すること
を特徴とする磁気共鳴イメージング装置。 - 請求項1記載の磁気共鳴イメージング装置であって、
前記事前処理部は、前記各ハーフRFパルスの照射周波数をそれぞれ前記補正値としてさらに算出する照射周波数算出部をさらに備え、
前記照射周波数算出部は、前記2回のスライス選択励起による励起位置間の位置ずれを解消するよう前記各照射周波数を算出すること
を特徴とする磁気共鳴イメージング装置。 - 請求項1記載の磁気共鳴イメージング装置であって、
前記事前処理部は、前記正極データと前記負極データとの間の位相差の0次項である0次位相差を前記補正値としてさらに算出する0次位相差算出部をさらに備え、
前記画像再構成部は、加算前に、前記正極データと前記負極データとの間の位相差を、前記0次位相差を用いて補正すること
を特徴とする磁気共鳴イメージング装置。 - 請求項1記載の磁気共鳴イメージング装置であって、
前記事前処理部は、
前記各ハーフRFパルスの照射周波数をそれぞれ前記補正値としてさらに算出する照射周波数算出部と、
前記正極データと前記負極データとの間の位相差の0次項である0次位相差を前記補正値としてさらに算出する0次位相差算出部と、をさらに備え、
前記照射周波数算出部は、前記2回のスライス選択励起による励起位置間の位置ずれを解消するよう前記各照射周波数を算出し、
前記画像再構成部は、加算前に、前記正極データと前記負極データとの間の位相差を、前記0次位相差を用いて補正すること
を特徴とする磁気共鳴イメージング装置。 - 請求項1乃至4のいずれか一項記載の磁気共鳴イメージング装置であって、
前記事前処理部は、前記パルスシーケンスのスライス傾斜磁場波形を測定するスライス傾斜磁場波形測定部をさらに備え、
前記リフォーカスパルス印加量算出部は、前記測定したスライス傾斜磁場波形を用い、前記各リフォーカスパルスの印加量を算出すること
を特徴とする磁気共鳴イメージング装置。 - 請求項2又は4記載の磁気共鳴イメージング装置であって、
前記事前処理部は、前記パルスシーケンスのスライス傾斜磁場波形を測定するスライス傾斜磁場波形測定部をさらに備え、
前記リフォーカスパルス印加量算出部は、前記測定したスライス傾斜磁場波形を用い、前記各リフォーカスパルスの印加量を算出し、
前記照射周波数算出部は、前記測定したスライス傾斜磁場波形から得られるスライス傾斜磁場の強度を用い、前記位置ずれを算出すること
を特徴とする磁気共鳴イメージング装置。 - 請求項3又は4記載の磁気共鳴イメージング装置であって、
前記事前処理部は、前記パルスシーケンスのスライス傾斜磁場波形を測定するスライス傾斜磁場波形測定部をさらに備え、
前記リフォーカスパルス印加量算出部は、前記測定したスライス傾斜磁場波形を用い、前記各リフォーカスパルスの印加量を算出し、
前記0次位相差算出部は、前記極性が正極のスライス傾斜磁場波形と前記極性が負極のスライス傾斜磁場波形との差を用いて前記0次位相差を算出すること
を特徴とする磁気共鳴イメージング装置。 - 請求項1記載の磁気共鳴イメージング装置であって、
前記事前処理部は、
前記正極データおよび前記負極データそれぞれの励起プロファイルを測定する励起プロファイル測定部と、
前記それぞれの励起プロファイルを用い、前記位相差の1次項の係数を1次位相差として算出する1次位相差算出部と、をさらに備え、
前記リフォーカスパルス印加量算出部は、前記1次位相差を用いて前記各リフォーカスパルス印加量を決定すること
を特徴とする磁気共鳴イメージング装置。 - 請求項2記載の磁気共鳴イメージング装置であって、
前記事前処理部は、
前記正極データおよび前記負極データそれぞれの励起プロファイルを測定する励起プロファイル測定部と、
前記それぞれの励起プロファイルを用い、前記位相差の1次項の係数を1次位相差として算出する1次位相差算出部と、
前記励起プロファイル間の励起位置のシフト量を算出するシフト量算出部と、をさらに備え、
前記リフォーカスパルス印加量算出部は、前記1次位相差を用いて前記各リフォーカスパルス印加量を決定し、
前記照射周波数算出部は、前記シフト量を用いて前記位置ずれを決定すること
を特徴とする磁気共鳴イメージング装置。 - 請求項3記載の磁気共鳴イメージング装置であって、
前記事前処理部は、
前記正極データおよび前記負極データそれぞれの励起プロファイルを測定する励起プロファイル測定部と、
前記それぞれの励起プロファイルを用い、前記位相差の1次項の係数を1次位相差として算出する1次位相差算出部と、をさらに備え、
前記リフォーカスパルス印加量算出部は、前記1次位相差を用いて前記各リフォーカスパルス印加量を決定し、
前記0次位相差算出部は、前記それぞれの励起プロファイルを用い、前記0次位相差を算出すること
を特徴とする磁気共鳴イメージング装置。 - 請求項4記載の磁気共鳴イメージング装置であって、
前記事前処理部は、
前記正極データおよび前記負極データそれぞれの励起プロファイルを測定する励起プロファイル測定部と、
前記それぞれの励起プロファイルを用い、前記位相差の1次項の係数を1次位相差として算出する1次位相差算出部と、
前記励起プロファイル間の励起位置のシフト量を算出するシフト量算出部と、をさらに備え、
前記リフォーカスパルス印加量算出部は、前記1次位相差を用いて前記各リフォーカスパルス印加量を決定し、
前記照射周波数算出部は、前記シフト量を用いて前記位置ずれを決定し、
前記0次位相差算出部は、前記それぞれの励起プロファイルを用い、前記0次位相差を算出すること
を特徴とする磁気共鳴イメージング装置。 - 請求項1項記載の磁気共鳴イメージング装置であって、
前記事前処理部は、
前記正極データおよび前記負極データそれぞれの励起プロファイルを測定する励起プロファイル測定部と、
前記正極データと前記負極データとの間の位相差の1次項の係数である1次位相差と、当該位相差の0次項である0次位相差とを、予め定めた規則に従って予め定めた初期値から変化させ、評価値を最小にする値をそれぞれ探索し、当該1次位相差および当該0次位相差の最適値を決定する位相差最適値探索部と、をさらに備え、
前記評価値は、前記それぞれの励起プロファイルから得られるサイドローブの信号量であり、
前記リフォーカスパルス印加量算出部は、前記1次位相差を用いて前記各リフォーカスパルス印加量を決定し、
前記画像再構成部は、前記加算前に前記正極データと負極データとの間の位相差を、前記0次位相差の最適値を用いて補正すること
を特徴とする磁気共鳴イメージング装置。 - 請求項12記載の磁気共鳴イメージング装置であって、
前記位相差最適値探索部は、前記0次位相差を当該0次位相差の最適値に固定し、予め定められた規則に従って前記1次位相差を変化させて得た前記評価値を最小とする1次位相差を、前記1次位相差の最適値と決定し、前記1次位相差を当該1次位相差の最適値に固定し、予め定めた規則に従って前記0次位相差を変化させて得た前記評価値を最小とする0次位相差を、前記0次位相差の最適値と決定する処理を、当該0次位相差の最適値を得た際の評価値が予め定めた範囲に収束するまで行うこと
を特徴とする磁気共鳴イメージング装置。 - 請求項8記載の磁気共鳴イメージング装置であって、
前記事前処理部は、前記1次位相差算出部が前記1次位相差を算出する毎に、当該1次位相差が予め定めた収束条件を満足するか否かを判別する収束判別部をさらに備え、
前記判別結果が否である場合、前記リフォーカスパルス印加量算出部に前記印加量を算出させ、前記励起プロファイル測定部に算出した前記印加量を用いた場合の前記各励起プロファイルを測定させ、当該測定結果から前記1次位相差算出部に前記1次位相差を算出させること
を特徴とする磁気共鳴イメージング装置。 - 請求項9記載の磁気共鳴イメージング装置であって、
前記事前処理部は、前記1次位相差算出部および前記シフト量算出部がそれぞれ前記1次位相差および前記シフト量を算出する毎に、当該1次位相差および当該シフト量が予め定めた収束条件を満足するか否かを判別する収束判別部をさらに備え、
前記判別結果が否である場合、前記リフォーカスパルス印加量算出部に前記印加量を算出させるとともに前記照射周波数算出部に前記照射周波数を算出させ、前記励起プロファイル測定部に算出した前記印加量および前記照射周波数を用いた場合の前記各励起プロファイルを測定させ、当該測定結果から前記1次位相差算出部に前記1次位相差を算出させるとともに前記シフト量算出部に前記シフト量を算出させること
を特徴とする磁気共鳴イメージング装置。 - 請求項10記載の磁気共鳴イメージング装置であって、
前記事前処理部は、前記1次位相差算出部が前記1次位相差を算出する毎に、当該1次位相差が予め定めた収束条件を満足するか否かを判別する収束判別部をさらに備え、
前記判別結果が否である場合、前記リフォーカスパルス印加量算出部に前記印加量を算出させ、前記励起プロファイル測定部に算出した前記印加量を用いた場合の前記各励起プロファイルを測定させ、当該測定結果から前記1次位相差算出部に前記1次位相差を算出させ、
前記判別結果が前記収束条件を満足するものである場合、前記0次位相差算出部に最新の前記各励起プロファイルから前記0次位相差を算出させること
を特徴とする磁気共鳴イメージング装置。 - 請求項11記載の磁気共鳴イメージング装置であって、
前記事前処理部は、前記1次位相差算出部および前記シフト量算出部がそれぞれ前記1次位相差および前記シフト量を算出する毎に、当該1次位相差および当該シフト量が予め定めた収束条件を満足するか否かを判別する収束判別部をさらに備え、
前記判別結果が否である場合、前記リフォーカスパルス印加量算出部に前記印加量を算出させるとともに前記照射周波数算出部に前記照射周波数を算出させ、前記励起プロファイル測定部に算出した前記印加量および前記照射周波数を用いた場合の前記各励起プロファイルを測定させ、当該測定結果から前記1次位相差算出部に前記1次位相差を算出させるとともに前記シフト量算出部に前記シフト量を算出させ、
前記判別結果が前記収束条件を満足するものである場合、前記0次位相差算出部に、最新の前記各励起プロファイルから前記0次位相差を算出させること
を特徴とする磁気共鳴イメージング装置。 - 請求項4記載の磁気共鳴イメージング装置であって、
前記本計測は、マルチスライス計測であって、
前記事前処理部は、計測対象スライス位置毎に、前記本計測に用いる前記リフォーカスパルスの印加量、前記照射周波数、および、前記0次位相差を決定すること
を特徴とする磁気共鳴イメージング装置。 - ハーフRFパルスとともに印加するスライス傾斜磁場の極性を正極と負極との間で反転させて2回のスライス選択励起を行い、それぞれエコー信号を取得する超短エコー時間シーケンスによる撮影に用いる補正値を算出する補正値算出方法であって、
前記補正値を決定する事前処理ステップと、
前記事前処理ステップで決定した補正値を用いて前記超短エコー時間シーケンスを実行し、前記スライス傾斜磁場を正極で印加した際に得たエコー信号である正極データと、前記スライス傾斜磁場を負極で印加した際に得たエコー信号である負極データとを得る計測ステップと、
前記正極データと前記負極データとを加算し、加算後の極性加算データを用い画像を再構成する画像再構成ステップと、を備え、
前記事前処理ステップは、前記スライス傾斜磁場をリフォーカスするリフォーカスパルスの印加量を前記補正値として決定するリフォーカスパルス印加量決定ステップを備え、 前記リフォーカスパルス印加量決定ステップでは、前記リフォーカスパルスの印加量は、前記正極データと前記負極データとを加算した後の励起プロファイルのサイドローブ信号を低減させるよう決定されること
を特徴とする補正値算出方法。 - 請求項19記載の補正値算出方法であって、
前記事前処理ステップは、
前記各ハーフRFパルスの照射周波数をそれぞれ前記補正値として算出する照射周波数算出ステップと、
前記正極データと前記負極データとの間の位相差の0次項である0次位相差を前記補正値として算出する0次位相差算出ステップと、をさらに備え、
前記照射周波数算出ステップは、前記2回のスライス選択励起位置の位置ずれを解消するよう前記各照射周波数を算出し
前記画像再構成ステップでは、前記加算前に前記正極データと負極データとの間の位相差は、前記0次位相差を用いて補正されること
を特徴とする補正値算出方法。
Priority Applications (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US14/232,470 US9594140B2 (en) | 2011-08-23 | 2012-08-21 | Magnetic resonance imaging apparatus and method for calculating correction value as application amount of refocusing pulse for UTE sequence |
JP2013530017A JP5984816B2 (ja) | 2011-08-23 | 2012-08-21 | 磁気共鳴イメージング装置および補正値算出方法 |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2011181739 | 2011-08-23 | ||
JP2011-181739 | 2011-08-23 |
Publications (1)
Publication Number | Publication Date |
---|---|
WO2013027710A1 true WO2013027710A1 (ja) | 2013-02-28 |
Family
ID=47746449
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/JP2012/071020 WO2013027710A1 (ja) | 2011-08-23 | 2012-08-21 | 磁気共鳴イメージング装置および補正値算出方法 |
Country Status (3)
Country | Link |
---|---|
US (1) | US9594140B2 (ja) |
JP (1) | JP5984816B2 (ja) |
WO (1) | WO2013027710A1 (ja) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN112014780A (zh) * | 2019-05-31 | 2020-12-01 | 西门子(深圳)磁共振有限公司 | 局部线圈及磁共振成像系统 |
Families Citing this family (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE102013219753B4 (de) * | 2013-09-30 | 2015-04-09 | Siemens Aktiengesellschaft | Korrektur von mittels Magnetresonanztechnik aufgenommenen Messdaten durch eine Ent-Faltung der Messdaten |
RU2689974C2 (ru) * | 2014-09-18 | 2019-05-29 | Конинклейке Филипс Н.В. | Способ генерации многодиапазонных рч импульсов |
CN107209236B (zh) * | 2015-02-02 | 2020-08-04 | 皇家飞利浦有限公司 | 用于确定mr系统的性能退化的mr指纹识别 |
DE102015223658B4 (de) * | 2015-11-30 | 2017-08-17 | Siemens Healthcare Gmbh | Verfahren zum Erfassen von Magnetresonanz-Signalen eines Untersuchungsobjekts |
EP3663786A1 (en) * | 2018-12-05 | 2020-06-10 | Siemens Healthcare GmbH | Normalized mr relaxation parameter |
CN109793518B (zh) * | 2019-01-24 | 2022-08-26 | 奥泰医疗系统有限责任公司 | 一种磁共振b0场图测量方法 |
DE102020206515A1 (de) * | 2020-05-26 | 2021-12-02 | Siemens Healthcare Gmbh | Sättigungspräparierte Aufnahme von MR-Bilddaten |
Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH02211124A (ja) * | 1989-02-13 | 1990-08-22 | Hitachi Medical Corp | 磁気共鳴イメージング装置 |
JPH04135539A (ja) * | 1990-09-27 | 1992-05-11 | Toshiba Corp | 磁気共鳴アンギオグラフィ装置 |
WO2004095049A1 (en) * | 2003-04-24 | 2004-11-04 | Medical Research Council | Phosphorus magnetic resonance imaging |
WO2010074057A1 (ja) * | 2008-12-26 | 2010-07-01 | 株式会社 日立メディコ | 磁気共鳴イメージング装置及びパルスシーケンス調整方法 |
Family Cites Families (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4812760A (en) * | 1987-07-27 | 1989-03-14 | General Electric Company | Multi-dimensional selective NMR excitation with a single RF pulse |
DE3823398A1 (de) * | 1988-07-09 | 1990-01-11 | Spectrospin Ag | Verfahren zur erzeugung einer folge von spinechosignalen, die verwendung dieses verfahrens bei der kernspintomographie und vorrichtung zum durchfuehren bzw. zur verwendung dieses verfahrens |
US5025216A (en) * | 1989-07-28 | 1991-06-18 | The Board Of Trustees Of The Leland Stanford Junior University | Magnetic resonance imaging of short T2 species |
JPH0435539A (ja) | 1990-05-31 | 1992-02-06 | Nec Corp | 広域多者間会議システム |
JP2003517321A (ja) * | 1997-10-07 | 2003-05-27 | ザ ボード オブ トラスティーズ オブ ザ リーランド スタンフォード ジュニア ユニバーシティ | 器具コントラストの調整を与える介在性器具の視角傾斜イメージングのための方法。 |
US7166998B2 (en) * | 2003-12-12 | 2007-01-23 | The Trustees Of The University Of Pennsylvania | Exact half pulse synthesis via the inverse scattering transform |
US7479783B2 (en) * | 2006-11-15 | 2009-01-20 | Beth Israel Deaconess Medical Center, Inc. | Echo train preparation for fast spin-echo acquisition |
-
2012
- 2012-08-21 US US14/232,470 patent/US9594140B2/en active Active
- 2012-08-21 JP JP2013530017A patent/JP5984816B2/ja active Active
- 2012-08-21 WO PCT/JP2012/071020 patent/WO2013027710A1/ja active Application Filing
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH02211124A (ja) * | 1989-02-13 | 1990-08-22 | Hitachi Medical Corp | 磁気共鳴イメージング装置 |
JPH04135539A (ja) * | 1990-09-27 | 1992-05-11 | Toshiba Corp | 磁気共鳴アンギオグラフィ装置 |
WO2004095049A1 (en) * | 2003-04-24 | 2004-11-04 | Medical Research Council | Phosphorus magnetic resonance imaging |
WO2010074057A1 (ja) * | 2008-12-26 | 2010-07-01 | 株式会社 日立メディコ | 磁気共鳴イメージング装置及びパルスシーケンス調整方法 |
Non-Patent Citations (2)
Title |
---|
C. SCHROEDER ET AL.: "Slice Excitation for Ultrashort TE Imaging", PROC. INTL. SOC. MAG. RESON. MED., vol. 12, May 2004 (2004-05-01) * |
M. TAKIZAWA ET AL.: "Correcting K-trajectory by Using Multiple Function Models of Gradient Waveform for Ultrashort TE(UTE)", PROC. INTL. SOC. MAG. RESON. MED., vol. 19, May 2011 (2011-05-01) * |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN112014780A (zh) * | 2019-05-31 | 2020-12-01 | 西门子(深圳)磁共振有限公司 | 局部线圈及磁共振成像系统 |
US11550007B2 (en) | 2019-05-31 | 2023-01-10 | Siemens Healthcare Gmbh | Local coil and magnetic resonance imaging system |
CN112014780B (zh) * | 2019-05-31 | 2023-06-27 | 西门子(深圳)磁共振有限公司 | 局部线圈及磁共振成像系统 |
Also Published As
Publication number | Publication date |
---|---|
JPWO2013027710A1 (ja) | 2015-03-19 |
US20140167752A1 (en) | 2014-06-19 |
JP5984816B2 (ja) | 2016-09-06 |
US9594140B2 (en) | 2017-03-14 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
JP5984816B2 (ja) | 磁気共鳴イメージング装置および補正値算出方法 | |
US7944209B2 (en) | Magnetic resonance imaging apparatus and method | |
US8587306B2 (en) | Magnetic resonance imaging apparatus and multi-contrast acquiring method | |
KR101663365B1 (ko) | 자기 공명 제어 시퀀스 결정 | |
JP6120806B2 (ja) | 金属物体を含むターゲット範囲の磁気共鳴データの取得方法および磁気共鳴装置 | |
JP6071905B2 (ja) | 磁気共鳴イメージング装置及び領域撮像方法 | |
EP2526440B1 (en) | Susceptibility gradient mapping | |
JP5730214B2 (ja) | 磁気共鳴イメージング装置及び2次元励起調整方法 | |
JP6417406B2 (ja) | 強調磁化率コントラストによるmrイメージング | |
JP2003225223A (ja) | 磁気共鳴イメージング装置 | |
WO2015033779A1 (ja) | 磁気共鳴イメージング装置および磁気共鳴イメージング方法 | |
JP5823865B2 (ja) | 磁気共鳴イメージング装置および照射周波数調整方法 | |
JPWO2012026382A1 (ja) | 磁気共鳴イメージング装置及び振動誤差磁場低減方法 | |
JP6013161B2 (ja) | 磁気共鳴イメージング装置および磁気共鳴イメージング方法 | |
JP5237957B2 (ja) | 磁気共鳴撮影装置 | |
WO2016021603A1 (ja) | 磁気共鳴イメージング装置および磁気共鳴イメージング方法 | |
JP4781120B2 (ja) | 磁気共鳴撮影装置および磁気共鳴スペクトル計測方法 | |
US10162027B2 (en) | Magnetic resonance imaging apparatus and irradiation magnetic field distribution measurement method | |
WO2013046900A1 (ja) | 磁気共鳴撮像装置、高周波磁場照射方法およびプログラム | |
JP2018114163A (ja) | 磁気共鳴イメージング装置 | |
JP6513493B2 (ja) | 磁気共鳴撮像装置 |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
121 | Ep: the epo has been informed by wipo that ep was designated in this application |
Ref document number: 12825998 Country of ref document: EP Kind code of ref document: A1 |
|
ENP | Entry into the national phase |
Ref document number: 2013530017 Country of ref document: JP Kind code of ref document: A |
|
WWE | Wipo information: entry into national phase |
Ref document number: 14232470 Country of ref document: US |
|
NENP | Non-entry into the national phase |
Ref country code: DE |
|
122 | Ep: pct application non-entry in european phase |
Ref document number: 12825998 Country of ref document: EP Kind code of ref document: A1 |