MRI approach of multiple times to repeat for detection of neuronal oscillations
11185248 · 2021-11-30
Assignee
Inventors
- Sung-Hong Park (Daejeon, KR)
- Kihwan KIM (Daejeon, KR)
- Hyoim Heo (Daejeon, KR)
- Hyun-Soo Lee (Daejeon, KR)
Cpc classification
A61B5/055
HUMAN NECESSITIES
International classification
A61B5/055
HUMAN NECESSITIES
Abstract
Disclosed are a method of detecting a neuron resonance signal and an MRI signal processing apparatus. The method of detecting a neuron resonance signal includes acquiring a plurality of different digital sequences respectively corresponding to a plurality of different repetition periods by sampling a magnetic resonance signal of a neuron resonance signal according to each of the plurality of different repetition periods and calculating correlation between the plurality of different digital sequences in a frequency band based on the plurality of different digital sequences.
Claims
1. A method of detecting a neuron resonance signal, the method comprising: acquiring a plurality of first digital sequences corresponding to a first period by sampling a magnetic resonance signal of the neuron resonance signal according to the first period; acquiring a plurality of second digital sequences corresponding to a second period by sampling the magnetic resonance signal of the neuron resonance signal according to the second period, wherein the second period is different from the first period; calculating a correlation between the first digital sequences and the second digital sequences; and identifying a frequency component of the neuronal resonance signal based on the calculated correlation.
2. The method as claimed in claim 1, further comprising: identifying a frequency component in which a magnitude of the calculated correlation is equal to or greater than a predetermined magnitude, as the frequency component of the neuron resonance signal.
3. The method as claimed in claim 1, wherein the calculating comprises calculating the correlation by transforming each of the first and second digital sequences into a frequency band and superpositioning the first and second digital sequences of the transformed frequency bands.
4. The method as claimed in claim 1, wherein the calculating comprises calculating the correlation by convoluting the first digital sequences with the second digital sequences and transforming the convoluted first and second digital sequences into frequency bands.
5. The method as claimed in claim 1, wherein the calculating comprises setting a certain resonance frequency and calculating the correlation based on the set certain resonance frequency, a phase difference between each of the first and second periods, and data of each of the acquired first and second digital sequences.
6. The method as claimed in claim 1, further comprising: padding dummy data to each of the acquired first and second digital sequences to become a preset sampling period.
7. The method as claimed in claim 6, wherein the dummy data is 0, a predetermined constant, or a value acquired by interpolating data included in each of the first and second digital sequences.
8. The method as claimed in claim 1, wherein the first digital sequences are generated from a first read-out sequence representing a magnitude of the neuron resonance signal acquired at each read-out time point of the magnetic resonance signal according to the first period, and the second digital sequences are generated from a second read-out sequence representing a magnitude of the neuron resonance signal acquired at each read-out time point of the magnetic resonance signal according to the second period.
9. The method as claimed in claim 8, wherein the first digital sequences are sequences generated by padding first dummy data to the first read-out sequence to make the sampling period be a predetermined period, and the second digital sequences are sequences generated by padding second dummy data to the second read-out sequence such that the sampling period is the predetermined period.
10. The method as claimed in claim 9, wherein the calculating comprises calculating the correlation by superpositioning the first frequency spectrum of the first digital sequences and the second frequency spectrum of the second digital sequences.
11. The method as claimed in claim 9, wherein the calculating comprises convoluting the first digital sequences and the second digital sequences, transforming the convoluted first and second digital sequences into a frequency band, and calculating the correlation from a frequency spectrum of the convoluted first and second digital sequences.
12. The method as claimed in claim 9, wherein the predetermined period is equal to or smaller than a difference value between the first period and the second period.
13. A magnetic resonance imaging (MRI) signal processing apparatus comprising: an input unit receiving a magnetic resonance signal of a neuron resonance signal; and a controller acquiring a plurality of different digital sequences respectively corresponding to a plurality of different repetition periods by sampling the magnetic resonance signal of the neuron resonance signal according to each of the plurality of different repetition periods, wherein the controller: calculates correlation between the plurality of different digital sequences in a frequency band based on the plurality of different digital sequences, and identifies a frequency component of the neuronal resonance signal based on the calculated correlation.
14. A non-transitory computer-readable medium records a program executing: acquiring a plurality of first digital sequences corresponding to a first period by sampling a magnetic resonance signal of the neuron resonance signal according to the first period; acquiring a plurality of second digital sequences corresponding to a second period by sampling the magnetic resonance signal of the neuron resonance signal according to the second period, wherein the second period is different from the first period; calculating a correlation between the first digital sequences and the second digital sequences; and identifying a frequency component of the neuronal resonance signal based on the calculated correlation.
Description
BRIEF DESCRIPTION OF THE DRAWING FIGURES
(1) The above and/or other aspects of the present invention will be more apparent by describing certain exemplary embodiments of the present invention with reference to the accompanying drawings, in which:
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DETAILED DESCRIPTION OF THE EXEMPLARY EMBODIMENTS
(16) The exemplary embodiments of the present invention may be diversely modified. Accordingly, specific exemplary embodiments are illustrated in the drawings and are described in detail in the detailed description. The matters defined in the description, such as detailed construction and elements, are provided to assist in a comprehensive understanding of the invention. Thus, it is apparent that the exemplary embodiments of the present invention may be carried out without those specifically defined matters. Also, well-known functions or constructions are not described in detail since they would obscure the invention with unnecessary detail.
(17) The terms “first”, “second”, etc. may be used to describe diverse components, but the components are not limited by the terms. The terms are only used to distinguish one component from the others.
(18) The terms used in the present application are only used to describe the exemplary embodiments but are not intended to limit the scope of the invention. The singular expression also includes the plural meaning as long as it does not differently mean in the context. In the present application, the terms “include” and “consist of” designates the presence of features, numbers, steps, operations, components, elements, or a combination thereof that are written in the specification but does not exclude the presence or possibility of addition of one or more other features, numbers, steps, operations, components, elements, or a combination thereof. It will be understood that when an element is referred to as being “connected” or “coupled” to another element, it can be directly connected or coupled to the other element or intervening elements may be present. In contrast, when an element is referred to as being “directly connected” or “directly coupled” to another element, there are no intervening elements present.
(19) In the exemplary embodiment of the present invention, a “module” or a “unit” performs at least one function or operation, and may be implemented with hardware, software, or a combination of hardware and software. In addition, a plurality of “modules” or a plurality of “units” may be integrated into at least one module except for a “module” or a “unit” which has to be implemented with specific hardware and may be implemented with at least one controller. As used herein, the singular forms “a,”, “an” and “the” are intended to include the plural forms as well, unless the context clearly indicates otherwise.
(20) The exemplary embodiments of the present invention will now be described in greater detail with reference to the accompanying drawings. In the following description, same drawing reference numerals are used for the same elements even in different drawings. Thus, description of the same elements is not repeated.
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(22) The brain of mammals exhibits resonance within a group of neurons by the interaction between neurons. As illustrated in
(23) The present invention provides a neuron resonance magnetic resonance imaging (NR-MRI) capable of measuring frequency-selective communication signals between brain regions. The present invention also provides a method of extracting a resonance frequency component inherent to neurons to provide an NR-MRI.
(24) A resonance frequency component inherent to neurons may be identified by sampling a magnetic resonance signal of a neuron resonance signal and using the sampled magnetic resonance signal. That is, the magnetic resonance signal may be the same signal as the neuron resonance signal. A frequency of the neuron resonance signal is higher than a frequency at which the neuron resonance signal can be sampled by the present technology. For example, the frequency at which the neuron resonance signal can be sampled is 5 Hz or less, but the frequency of the neuron resonance signal is about tens of Hz. According to the Nyquist Theorem, data must be sampled based on a frequency at least twice a highest frequency of an input signal to restore the original analog signal without loss. However, as described above, since the frequency that can be sampled is lower than the frequency of the neuron resonance signal, the resonance frequency component inherent to neurons may not be identified only by the general sampling method. Thus, Korean Patent Registration No. 10-1683217 discloses a method of extracting a resonance frequency of neurons by assuming a resonance frequency of neurons as a specific value. However, since the resonance frequency of neurons differs according to brain regions, the aforementioned method may extract the resonance frequency of neurons in a specific region but has limitations in extracting the resonance frequency of neurons included in all brain regions. Thus, the present invention provides a general method of extracting the resonance frequency of neurons for all brain regions.
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(27) Hereinafter, a method of acquiring a frequency component of a neuron resonance signal according to an exemplary embodiment of the present invention will be described with reference to
(28) Referring to
(29) Thereafter, the MRI controller may acquire first observation values a11, a12, a13, a14, . . . regarding a magnitude of the neuron resonance signal 1 of neurons to be observed at time points t11, t12, t13, and t14, which have elapsed by a predetermined value from time points at which the respective RF excitation signals e11, e12, e13, and e14, . . . were generated.
(30) The time points (t11, t12, t13, and t14, . . . ) that have elapsed by a predetermined value may be referred to as read-out time points in this disclosure. Here, the predetermined value may correspond to a time echo (TE).
(31) Discrete data formed by sequentially arranging the first observation values a11, a12, a13, a14, . . . acquired regarding the magnitude of the neuron resonance signal 1 may be referred to as a “first read-out sequence d11”. For example, the first read-out sequence d11 may be given as d11=[a11, a12, a13, a14, . . . ]. A process of acquiring the first read-out sequence d11 may be referred to as a first process P1 in this disclosure hereinafter. A first digital sequence may be generated by padding dummy data to the acquired first read-out sequence d11, and if the acquired first read-out sequence d11 is not padded with the dummy data, the first read-out sequence d11 may be a first digital sequence.
(32) Referring to
(33) Here, the second TR 21 may be a value different from the first TR 11. For example, if the first TR 11 is repeated at 20 Hz, the second TR 21 may be repeated at 21 Hz. However, these specific numerical values are merely an example, and the TRs may be set to various values.
(34) Thereafter, the MRI controller may acquire second observation values a21, a22, a23, a24, . . . regarding a magnitude of the neuron resonance signal 1 of neurons to be observed at time points t21, t22, t23, and t24, which have elapsed by a predetermined value from time points at which the respective RF excitation signals e21, e22, e23, and e24, . . . were generated.
(35) Discrete data formed by sequentially arranging the second observation values a21, a22, a23, a24, . . . acquired regarding the magnitude of the neuron resonance signal 1 may be referred to as a “second read-out sequence d21”. For example, the second read-out sequence d21 may be given as d21=[a21, a22, a23, a24, . . . ]. A process of acquiring the second read-out sequence d21 may be referred to as a second process P2 in this disclosure hereinafter. A second digital sequence may be generated by padding dummy data to the acquired second read-out sequence d21, and if the acquired second read-out sequence d21 is not padded with the dummy data, the second read-out sequence d21 may be a second digital sequence.
(36) In
(37) Meanwhile,
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(39) Referring to
(40) Based on the plurality of different digital sequences, the MRI signal processing apparatus calculates correlation between the plurality of different digital sequences in a frequency band (S420). For example, the MRI signal processing apparatus may transform each of the plurality of different digital sequences into a frequency band and superposition the plurality of different digital sequences of the transformed frequency bands to calculate correlation. Alternatively, the MRI signal processing apparatus may convolute the plurality of different digital sequences and transform the convoluted digital sequences into frequency bands to calculate correlation.
(41) The MRI signal processing apparatus may set a certain resonance frequency of the neuron resonance signal and calculate correlation based on phase differences between the set certain resonance frequency and each of the different repetition periods and data of the plurality of acquired different digital sequences. In an exemplary embodiment, in case where the resonance frequency f.sub.NO of the neuron resonance signal is assumed to be 20 Hz, the period TNO is 50 ms. If the first TR is 60 ms, data sampled consecutively according to the first TR is data at the moments of T.sub.NO+10 ms, T.sub.NO+20 ms, T.sub.NO+30 ms, . . . , T.sub.NO+(10×n)ms. If the second TR is 50 ms, the data continuously sampled according to the second TR is data at the moments of T.sub.NO-10 ms, T.sub.NO-20 ms, T.sub.NO-30 ms, . . . , T.sub.NO-(10×n)ms. If the assumed resonance frequency of the neuron resonance signal matches a resonance frequency of an actual neuron resonance signal, energy in the frequency band of the data sampled according to the first TR and the second TR may be calculated to be larger than energy in the other bands. A specific process of calculating correlation between the plurality of different digital sequences by the MRI signal processing apparatus will be described hereinafter.
(42) Meanwhile, the MRI signal processing apparatus may identify a frequency component in which a magnitude of calculated correlation is greater than a predetermined magnitude, as a frequency component of the neuron resonance signal.
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(44) After it is assumed that a signal of neurons to be observed in the frequency component analysis method illustrated in
(45) The correlation calculation process PC may be performed a plurality of times and the value of the assumed resonance frequency may be changed each time the correlation calculation process PC is performed. When the value of the assumed resonance frequency is changed, correlation between the first read-out sequence d11 and the second read-out sequence d21 may also be changed. Here, the changed assumed resonance frequency values may be expressed, for example, as f1, f2, f3, f4, . . . . The assumed resonance frequency values may refer to a plurality of different TRs (repetition times or repetition periods).
(46) The present invention is provided for a situation in which the actual resonance frequency fr of the signal of the neuron is not known in advance. Therefore, which of the assumed resonance frequency values f1, f2, f3, f4, . . . . the actual resonance frequency fr is equal to or closest to may be detected according to exemplary embodiments of the present invention described hereinafter.
(47) Referring to
(48) In step S510, it is assumed that the resonance frequency of the neurons to be observed is a specific assumed resonance frequency fk (k=1, 2, 3, . . . , or x).
(49) Under the assumption in step S510, correlation CVk between the first read-out sequence d11 and the second read-out sequence d21 described above is acquired in step S520.
(50) The above-described steps S510 and S520 may be repeatedly performed, while changing the specific assumed resonance frequency fk to different values f1, f2, f3, . . . , fx. As a result, a set of correlations {CV1, CV2, CV3, . . . CVx} may be calculated.
(51) In step S530, a largest value among the set of correlations {CV1, CV2, CV3, . . . CVx} may be selected.
(52) In step S540, an assumed resonance frequency corresponding to the correlation selected from among the assumed resonance frequency values {f1, f2, f3, . . . , fx}.
(53) In step S550, it may be determined that the selected assumed resonance frequency is included in the resonance frequency of the neuron.
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(55) Referring to
(56) In step S530, values larger than a predetermined value may be selected from among the set of correlations {CV1, CV2, CV3, . . . CVx}.
(57) The first read-out sequence and the second read-out sequence may be acquired a plurality of times by performing the first process and the second process described above a plurality of times, respectively. Here, the SNR may be increased using the plurality of first read-out sequences and the plurality of second read-out sequences in the process of acquiring the correlation CVk. In
(58) According to an exemplary embodiment of the present invention, the method of calculating correlation between the first read-out sequence d11 and the second read-out sequence d21 may use a frequency spectrum correlation calculation process P3.
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(60) The frequency spectrum correlation calculation process P3 may be performed on the assumption that neurons to be observed resonates at a specific assumed resonance frequency.
(61) The frequency spectrum correlation calculating process P3 may include:
(62) Step S710: transforming the first read-out sequence into a frequency region to generate a first frequency spectrum f11, [94] Step S720: transforming the second read-out sequence into a frequency region to generate a second frequency spectrum f21, and [95] Step S730: calculating frequency region-correlation between the first frequency spectrum and the second frequency spectrum as correlation between the first read-out sequence and the second read-out sequence.
(63) Here, the method of calculating correlation between the first read-out sequence d11 and the second read-out sequence d21 may include performing the frequency spectrum correlation calculation process P3 one or more times, while changing the specific assumed resonance frequency. For example, the frequency spectrum correlation calculation process P3 may be performed on each frequency included in the predetermined assumed resonance frequency set {f1, f2, f3, . . . , fx}, and, as a result, a plurality of frequency region-correlations may be calculated.
(64) The frequency component analysis method of analyzing the frequency component of the neuron resonance signal illustrated in
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(66) In step S810, a value related to first energy of a specific assumed resonance frequency may be calculated in the first frequency spectrum.
(67) In step S820, a value related to the second energy of the specific assumed resonance frequency may be calculated in the second frequency spectrum.
(68) In step S830, a value acquired by superpositioning the first energy and the second energy may be calculated as a frequency region-correlation between the first frequency spectrum and the second frequency spectrum.
(69) Here, the ‘superpositioning’ in step S830 may be a process of reinforcing the first energy using the second energy, and reinforcing the first energy using the second energy may refer to calculation of combining the first energy and the second energy using a method of adding, multiplying, or the like, the first energy and the second energy. Here, the first read-out sequence may be acquired by sampling the neuron resonance signal at the first TR interval. The neuron resonance signal is assumed to resonate at a specific assumed resonance frequency. Also, the second read-out sequence may be acquired by sampling the neuron resonance signal at the second TR interval. The neuron resonance signal is assumed to resonate at a specific assumed resonance frequency.
(70) A person skilled in the art will understand that, when it is assumed that neurons to be observed resonate at a specific assumed resonance frequency, a first maximum frequency represented by the first frequency spectrum and a second maximum frequency represented by the second frequency spectrum may be varied according to sampled data based on each specific assumed resonance frequency value and the first TR or the second TR.
(71) For example, when it is assumed that the neuron resonance signal resonates at 50 Hz, the period of the neuron resonance signal is 20 ms.
(72) Here, when the first TR is 90 ms, a phase of the neuron resonance signal observed at each read-out time point is shifted by 10 ms, and here, the first maximum frequency of the first frequency spectrum is 1000/10 ms=100 Hz.
(73) When the second TR is 91 ms, the phase of the neuron resonance signal observed at each read-out time point is shifted by 9 ms, and the second maximum frequency of the second frequency spectrum is 1000/9 ms=˜111 Hz.
(74) When the first maximum frequency and the second maximum frequency are determined as described above, the value related to the first energy corresponding to 50 Hz, the specific assumed resonance frequency, may be found from the first frequency spectrum, and the value related to the second energy corresponding to 50 Hz, the specific assumed resonance frequency, may be found from the second frequency spectrum as presented in steps S810 and S820.
(75) Thereafter, as presented in step S830, the value acquired by superpositioning the first energy and the second energy may be calculated as a frequency region-correlation between the first frequency spectrum and the second frequency spectrum.
(76) Meanwhile, a first case where the specific assumed resonance frequency is the same as the actual resonance frequency at which the observed neurons resonate, and a second case where the specific assumed resonance frequency is not the same as the actual resonance frequency may be classified. For example, when actual resonance frequency of neurons is 50 Hz, a first case where the specific assumed resonance frequency is assumed to be 50 Hz and a second case were the specific assumed resonance frequency is 55 Hz may be classified.
(77) Here, the frequency region-correlation calculated in the first case may be larger than the frequency region-correlation calculated in the second case. Thus, it may be determined that the specific assumed resonance frequency 50 Hz is the actual resonance frequency in the first case which exhibits larger correlation.
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(82) In the second case of
(83) The MRI signal processing apparatus may detect first energy a3 corresponding to 55 Hz of the specific assumed resonance frequency in the first frequency spectrum and detects second energy a4 corresponding to 55 Hz of the specific assumed resonance frequency in the second frequency spectrum and superposition the first energy and the second energy to calculate a second superposition value a3*a4.
(84) As illustrated in
(85) A method of determining a resonance frequency of neurons according to another exemplary embodiment of the present invention will be described with reference to
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(87) In step S1110, the first read-out sequence d11=[a11, a12, a13, a14, . . . ] may be acquired using the first process P1 described above.
(88) In step S1120, the second read-out sequence d21=[a21, a22, a23, a24, . . . ] may be acquired using the second process P2 described above.
(89) In step S1130, a first digital sequence having a sampling interval ΔT may be generated from the first read-out sequence d11=[a11, a12, a13, a14, . . . ]. Meanwhile, step S1130 may include the following steps.
(90) In step S1131, first observation values a11, a12, a13, a14, . . . , which are respective elements of the first read-out sequence d11=[a11, a12, a13, a14, . . . ] may be arranged on the time axis. Here, a time interval between the first observation values adjacent to each other may be the same as the first TR 11.
(91) In step S1132, a first digital sequence may be generated by inserting first dummy data between the adjacent first observation values. Here, the first dummy data may be ‘0’ or a constant or may be values generated by interpolating first observation values arranged on a time axis. Here, a time interval of two elements adjacent to each other on the time axis, among the elements of the generated first digital sequence, may be set to ΔT. ΔT may be understood as a sampling interval.
(92) In step S1140, a second digital sequence having a sampling interval of ΔT may be generated from the second read-out sequence d21=[a21, a22, a23, a24, . . . ]. Meanwhile, step S1140 may include the following steps.
(93) In step S1141, the second observation values a21, a22, a23, a24, . . . , which are respective elements of the second read-out sequence d21=[a21, a22, a23, a24, . . . ] may be arranged on the time axis. Here, a time interval between the second observation values adjacent to each other may be the same as that of the second TR 21.
(94) In step S1142, a second digital sequence may be generated by inserting second dummy data between the adjacent second observation values. Here, the second dummy data may be ‘0’ or a constant or may be a value generated by interpolating the second observation values arranged on the time axis. Here, the time interval of two elements adjacent to each other on the time axis, among the elements of the generated second digital sequence, may be set to ΔT. ΔT may be understood as a sampling interval.
(95) Here, the maximum value of ΔT may be abs(first TR(11)−second TR(21)).
(96) In step S1150, the first digital sequence and the second digital sequence may be transformed into frequency regions to generate a first frequency spectrum and a second frequency spectrum, respectively. To this end, Fourier transform may be used. Here, the number of the first digital sequences used for the transform may be equal to the number of the second digital sequences used for the transform.
(97) In step S1160, the first frequency spectrum may be multiplied to the second frequency spectrum to generate a final frequency spectrum. Multiplying may mean that two spectrum values corresponding to the same frequency magnitude in the first and second frequency spectra are multiplied together.
(98) In step S1170, one or more frequency values having a magnitude equal to or greater than a threshold value may be selected from the final frequency spectrum, and one or more of the selected frequency values may be determined as a resonance frequency of neurons.
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(100) The first read-out sequence d11 sampled at the sampling rate TR1 on the time axis extending in the left and right direction of
(101) Here, a non-sampled space may be filled with 0 or interpolation.
(102) For example, in the case of TR1=90 ms and ΔT=1 ms, spaces between signal values acquired from the first read-out sequence d11 sampled at the sampling rate of TR1 may be filled with 89 dummy data ‘0’. The first frequency spectrum acquired by performing FFT on the first digital sequence acquired thusly may represent a frequency range of 0 to 500 Hz.
(103) For example, in the case of TR2=91 ms, ΔT=1 ms, spaces between signal values acquired from the second read-out sequence d21 sampled at the sampling rate TR2 may be filled with 90 dummy data ‘0’. The second frequency spectrum acquired by performing FFT on the second digital sequence acquired thusly may represent a frequency range of 0 to 500 Hz.
(104) Since the first digital sequence and the second digital sequence have more dummy data than the actually measured data, a large amount of aliased signals may appear in the calculated first frequency spectrum and second frequency spectrum. To suppress these aliased signals, the first frequency spectrum and the second frequency spectrum may be multiplied together to produce a final frequency spectrum. Accordingly, the frequency of neurons may be finally identified.
(105) In the method of filling spaces between data with dummy data ‘0’, the maximum value of ΔT may be the absolute value of TR1−TR2. That is, if TR1=90 ms, TR2=100 ms, ΔT may be a maximum of 10 ms, and in this case, spaces between the signals in the TR1 data may be filled with 8 dummy data ‘0’ each and spaces between the signals in TR2 data may be filled with 9 dummy data ‘0’ each. Thereafter, the ranges of the first frequency spectrum and the second frequency spectrum acquired after the Fourier transform may be all 0 to 50 Hz. Also, in this case, ΔT may be 1 ms. Here, preferably, ΔT is a divisor of 10 ms.
(106) A method of analyzing a frequency component of a neuron resonance signal provided according to various exemplary embodiments of the present invention may include the following steps.
(107) Descriptions will be given below with reference to
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(109) In step S1310, a first digital sequence may be generated from the first read-out sequence d11 indicating the magnitudes a101, a102, a03, a104, . . . of a neuron resonance signal 1 to be observed acquired at each of the read-out time points t11, t12, t13, . . . of the first MR sequence 10 having the first TR 11.
(110) In step S1320, a second digital sequence may be generated from the second read-out sequence d21 indicating the magnitudes a201, a202, a203, a204, . . . of the resonance signal 1 acquired at each of the read-out time points t21, t22, t23, . . . of the second MR sequence 20 having the second TR 21 different from the first TR 11.
(111) In operation S1330, a frequency component of the neuron resonance signal may be determined from a frequency spectrum generated by reinforcing the first frequency spectrum of the first digital sequence using the second frequency spectrum of the second digital sequence, or the frequency component of the neuron resonance signal may be identified from a frequency spectrum of a digital sequence generated by reinforcing the first digital sequence using the second digital sequence.
(112) Here, step S1310 may include step S1311 of generating a first digital sequence by padding the first dummy data to the first read-out sequence so that the sampling period of the first digital sequence is the predetermined ΔT.
(113) Step S1320 may include step S1321 of generating a second digital sequence by padding the second dummy data to the second read-out sequence so that the sampling period of the second digital sequence is ΔT.
(114) Also, in step S1330, the frequency component of the neuron resonance signal may be identified from a reinforced frequency spectrum generated by reinforcing the first frequency spectrum of the first digital sequence using the second frequency spectrum of the second digital sequence. Here, the reinforcing may be an addition or multiplication operation.
(115) Alternatively, in step S1330, the frequency component of the neuron resonance signal may be identified from the reinforced frequency spectrum generated by reinforcing the first digital sequence using the second digital sequence. Here, the reinforcing may be a convolution operation.
(116) The predetermined sampling period ΔT may be less than or equal to an absolute value of a difference between the first TR and the second TR. The first dummy data may be a value ‘0’, a constant, or a value interpolated from the first read-out sequence, and the second dummy data may be a value ‘0’, a constant, or a value interpolated from the second read-out sequence.
(117) A method of analyzing a frequency component of a neuron resonance signal provided according to another exemplary embodiment of the present invention may include the following steps.
(118) Descriptions will be given below with reference to
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(120) In step S1410, the first digital sequence may be generated from the first read-out sequence d11 indicating the magnitudes a101, a102, a103, a104 of the neuron resonance signal 1 to be observed, acquired at each of the read-out time points t11, t12, t13, . . . of the first MR sequence 10 having the first TR 11.
(121) In step S1420, the second digital sequence may be generated from the second read-out sequence d21 indicating the magnitudes a201, a202, a203, a204, . . . of the neuron resonance signal 1 acquired at each of the read-out time points t21, t22, t23, . . . of the second MR sequence 20 having the second TR 21 different from the first TR 11.
(122) In step S1430, the frequency component of the neuron resonance signal may be identified from the frequency spectrum generated by reinforcing the first frequency spectrum of the first digital sequence using the second frequency spectrum of the second digital sequence.
(123) Here, the first digital sequence may be a first read-out sequence, and the second digital sequence may be a second read-out sequence. In step S1430, the frequency component of the neuron resonance signal may be identified from the frequency spectrum generated by reinforcing the first frequency spectrum of the first digital sequence using the second frequency spectrum of the second digital sequence. Here, the reinforcing may be an addition or multiplication operation.
(124) Step S1430 may further include the following steps.
(125) In step S1431, assuming that the neurons to be observed resonate at one or more specific resonance frequencies, correlation between the first read-out sequence and the second read-out sequence for each specific assumed resonance frequency may be acquired.
(126) In step S1432, the frequency component of the neuron resonance signal may be detected based on one or more correlations acquired for one or more specific assumed resonance frequencies. Step S1432 may include step of selecting correlation having a value greater than or equal to a predetermined value among the one or more correlations (S1432-1) and identifying a frequency corresponding to the selected correlation, among the one or more specific assumed resonance frequencies, as a frequency included in the neuron resonance signal (S1432-2).
(127) Here, the MRI signal processing apparatus may acquire the first read-out sequence a plurality of times by performing S1410 step a plurality of times, acquire the second read-out sequence a plurality of times by performing step S1420 a plurality of times, and subsequently calculate correlation using the plurality of acquired first read-out sequences and the plurality of acquired second read-out sequences.
(128) Here, in step S1431, the frequency spectrum correlation including the following steps may be calculated. In step S1431-1, when the neurons to be observed are assumed to resonate at a specific resonance frequency, the first read-out sequence may be transformed into a frequency region to generate the first frequency spectrum. In step S1431-2, when the neurons to be observed are assumed to resonate at a specific resonance frequency, the second read-out sequence may be transformed into a frequency region to generate the second frequency spectrum. In step S1431-3, the frequency region-correlation between the first frequency spectrum and the second frequency spectrum may be calculated as correlation between the first read-out sequence and the second read-out sequence. In step S1431, the frequency spectrum correlation calculation process may be performed one or more times, while changing the assumed resonance frequency.
(129)
(130) Step S1510 may include the following steps S1511, S1512, and S1513. Step In S1511, a value regarding first energy of a specific resonance frequency may be calculated from the first frequency spectrum. In step S1512, a value regarding second energy of the specific resonance frequency may be calculated from the second frequency spectrum. In step S1513, a value acquired by reinforcing the first energy using the second energy may be calculated as a frequency region-correlation between the first frequency spectrum and the second frequency spectrum. Here, reinforcing may refer to an addition or multiplication operation.
(131) Referring back to
(132) Various exemplary embodiments of the method of detecting a neuron resonance signal have been described so far. Hereinafter, an MRI signal processing apparatus for detecting a neuron resonance signal will be described.
(133)
(134) Referring to
(135) The controller 120 samples the magnetic resonance signal of the neuron resonance signal according to each of a plurality of different repetition periods to acquire a plurality of different digital sequences respectively corresponding to the plurality of different repetition periods. The repetition period refers to a period for sampling the magnetic resonance signal of the neuron resonance signal at regular intervals and may also be expressed as a time to repetition (TR). The repetition period may include a first TR and a second TR, and may include a third TR, . . . , an n-th TR according to circumstances.
(136) The controller 120 calculates correlation between a plurality of different digital sequences in a frequency band based on a plurality of different digital sequences. The controller 120 may identify a frequency component in which a magnitude of the calculated correlation is equal to or greater than a predetermined magnitude, as a frequency component of the neuron resonance signal.
(137) Meanwhile, the controller 120 may transform each of the plurality of different digital sequences into a frequency band and may superposition the plurality of different digital sequences of the transformed frequency bands to calculate correlation. Alternatively, the controller 120 may convolute the plurality of different digital sequences and transform the convoluted digital sequences into frequency bands to calculate correlation.
(138) The controller 120 may pad the dummy data to a read-out sequence acquired from the neuron resonance signal at a predetermined period, to have a predetermined sampling period. For example, the dummy data may be 0, a predetermined constant, or a value acquired by interpolating data contained in a corresponding digital sequence.
(139) The controller 120 may set a certain resonance frequency of the neuron resonance signal and calculate correlation based on the set certain resonance frequency, a phase difference between the different repetition periods, and the plurality of different digital sequence data. Since specific exemplary embodiments have been described above, and thus, a description thereof will be omitted.
(140)
(141) Referring to
(142) Referring to
(143) The method of analyzing the neuron resonance signal according to various exemplary embodiments described above may be provided as a computer program product. The computer program product may include a software program itself or a non-transitory computer readable medium in which the software program is stored.
(144) The non-transitory computer readable medium is a medium that semi-permanently stores data therein, rather than storing data for a second such as a register, a cache, a memory, and the like, and is readable by a device. In detail, various applications or programs described above may be stored and provided in the non-transitory computer readable medium such as a compact disk (CD), a digital versatile disk (DVD), a hard disk, a Blu-ray disk, a universal serial bus (USB), a memory card, a read only memory (ROM), or the like.
(145) Although the exemplary embodiments have been illustrated and described hereinabove, the present disclosure is not limited to the above-mentioned specific exemplary embodiments but may be variously modified by those skilled in the art without departing from the scope and spirit of the present disclosure as disclosed in the accompanying claims. These modifications should also be understood to fall within the scope of the present disclosure. Further, using the exemplary embodiments of the present invention described above, those skilled in the art may easily make various changes and modifications within the scope of the present invention. The contents of each claim may be combined with other claims without a citing relationship within the scope that can be understood through this disclosure.