JPWO2021062154A5 - - Google Patents
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- JPWO2021062154A5 JPWO2021062154A5 JP2022515106A JP2022515106A JPWO2021062154A5 JP WO2021062154 A5 JPWO2021062154 A5 JP WO2021062154A5 JP 2022515106 A JP2022515106 A JP 2022515106A JP 2022515106 A JP2022515106 A JP 2022515106A JP WO2021062154 A5 JPWO2021062154 A5 JP WO2021062154A5
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Claims (32)
コンピュータによって、
測定デバイスまたはメモリから、前記サンプルに関連する磁気共鳴(MR)信号を取得することと、
コイル磁場基底ベクトルの所定のセットにアクセスすることであって、前記測定デバイス内のコイルのコイル感度が、前記係数を使用する前記コイル磁場基底ベクトルの所定のセットの加重重ね合わせによって表され、前記所定のコイル磁場基底ベクトルが、マクスウェル方程式の解である、アクセスすることと、
前記MR情報を入力として使用し、前記MR信号、前記係数、および前記コイル磁場基底ベクトルの所定のセットに対応する計算されたMR信号を出力するために前記サンプルの応答物理をシミュレートするフォワードモデルに少なくとも部分的に基づいて、前記サンプルに関連する前記MR情報および前記コイル感度の表現の前記係数の非線形最適化問題を解くことと、を含み、
前記MR情報が、前記MR信号によって指定される、前記サンプルと関連付けられたボクセル内の1つ以上のMRパラメータの定量値を含む、方法。 A method for determining coefficients of a coil sensitivity expression and MR information associated with a sample, the method comprising:
by computer,
obtaining a magnetic resonance (MR) signal associated with the sample from a measurement device or memory;
accessing a predetermined set of coil magnetic field basis vectors, wherein the coil sensitivity of a coil in the measuring device is represented by a weighted superposition of the predetermined set of coil magnetic field basis vectors using the coefficients; accessing a given coil magnetic field basis vector, which is a solution of Maxwell's equations;
a forward model that uses the MR information as input and simulates the response physics of the sample to output a calculated MR signal corresponding to a predetermined set of the MR signal , the coefficients, and the coil magnetic field basis vectors; solving a nonlinear optimization problem of the coefficients of the representation of the MR information and the coil sensitivity associated with the sample, based at least in part on
The method , wherein the MR information includes quantitative values of one or more MR parameters within voxels associated with the sample specified by the MR signal.
前記項が、前記測定デバイス内の前記コイルの前記コイル感度からの寄与を含む、請求項1に記載の方法。 the nonlinear optimization problem includes a term corresponding to the square of the absolute value of the difference between the MR signal and the estimated MR signal corresponding to the MR information;
2. The method of claim 1, wherein the term includes a contribution from the coil sensitivity of the coil within the measurement device.
前記1つ以上の制約は、前記MR情報の空間分布に対応する正則化子を含む、請求項1に記載の方法。 the nonlinear optimization problem includes one or more constraints on reduction or minimization of the term;
2. The method of claim 1, wherein the one or more constraints include a regularizer corresponding to a spatial distribution of the MR information.
測定デバイスと通信するように構成されたインターフェース回路と、
プログラム命令を記憶するように構成されたメモリと、
前記プログラム命令を実行するように構成されたプロセッサであって、前記プログラム命令が、前記プロセッサによって実行されるときに、前記コンピュータに、
前記測定デバイスまたは前記メモリから、サンプルに関連する磁気共鳴(MR)信号を取得することと、
コイル磁場基底ベクトルの所定のセットにアクセスすることであって、前記測定デバイス内のコイルのコイル感度が、前記係数を使用する前記コイル磁場基底ベクトルの所定のセットの加重重ね合わせによって表され、前記所定のコイル磁場基底ベクトルが、マクスウェル方程式の解である、アクセスすることと、
前記MR情報を入力として使用し、前記MR信号、前記係数、および前記コイル磁場基底ベクトルの所定のセットに対応する計算されたMR信号を出力するために前記サンプルの応答物理をシミュレートするフォワードモデルに少なくとも部分的に基づいて、前記サンプルに関連する前記MR情報および前記コイル感度の表現の前記係数の非線形最適化問題を解くことと、を含む動作を実施させる、プロセッサと、を備え、
前記MR情報が、前記MR信号によって指定される、前記サンプルと関連付けられたボクセル内の1つ以上のMRパラメータの定量値を含む、コンピュータ。 A computer,
an interface circuit configured to communicate with the measurement device;
a memory configured to store program instructions;
a processor configured to execute the program instructions, the program instructions, when executed by the processor, causing the computer to:
obtaining a magnetic resonance (MR) signal associated with the sample from the measurement device or the memory;
accessing a predetermined set of coil magnetic field basis vectors, wherein the coil sensitivity of a coil in the measuring device is represented by a weighted superposition of the predetermined set of coil magnetic field basis vectors using the coefficients; accessing a given coil magnetic field basis vector, which is a solution of Maxwell's equations;
a forward model that uses the MR information as input and simulates the response physics of the sample to output a calculated MR signal corresponding to a predetermined set of the MR signal , the coefficients, and the coil magnetic field basis vectors; a processor for performing operations comprising: solving a nonlinear optimization problem of the coefficients of the representation of the MR information and the coil sensitivity associated with the sample based at least in part on ;
The MR information includes quantitative values of one or more MR parameters within voxels associated with the sample specified by the MR signal.
前記項が、前記測定デバイス内の前記コイルの前記コイル感度からの寄与を含む、請求項13に記載のコンピュータ。 the nonlinear optimization problem includes a term corresponding to the square of the absolute value of the difference between the MR signal and the estimated MR signal corresponding to the MR information;
14. The computer of claim 13, wherein the term includes a contribution from the coil sensitivity of the coil within the measurement device.
測定デバイスまたはメモリから、サンプルに関連する磁気共鳴(MR)信号を取得することと、
コイル磁場基底ベクトルの所定のセットにアクセスすることであって、前記測定デバイス内のコイルのコイル感度が、前記係数を使用する前記コイル磁場基底ベクトルの所定のセットの加重重ね合わせによって表され、前記所定のコイル磁場基底ベクトルが、マクスウェル方程式の解である、アクセスすることと、
前記MR情報を入力として使用し、前記MR信号、前記係数、および前記コイル磁場基底ベクトルの所定のセットに対応する計算されたMR信号を出力するために前記サンプルの応答物理をシミュレートするフォワードモデルに少なくとも部分的に基づいて、前記サンプルに関連するMR情報および前記コイル感度の表現の前記係数の非線形最適化問題を解くことと、を含む動作を実施させ、
前記MR情報が、前記MR信号によって指定される、前記サンプルと関連付けられたボクセル内の1つ以上のMRパラメータの定量値を含む、非一時的なコンピュータ可読記憶媒体。 a non-transitory computer-readable storage medium for use in conjunction with a computer, the computer-readable storage medium configured to store program instructions, the program instructions, when executed by the computer; , to the computer,
obtaining a magnetic resonance (MR) signal associated with the sample from a measurement device or memory;
accessing a predetermined set of coil magnetic field basis vectors, wherein the coil sensitivity of a coil in the measuring device is represented by a weighted superposition of the predetermined set of coil magnetic field basis vectors using the coefficients; accessing a given coil magnetic field basis vector, which is a solution of Maxwell's equations;
a forward model that uses the MR information as input and simulates the response physics of the sample to output a calculated MR signal corresponding to a predetermined set of the MR signal , the coefficients, and the coil magnetic field basis vectors; solving a nonlinear optimization problem of the coefficients of the representation of the coil sensitivity and the MR information associated with the sample based at least in part on the MR information associated with the sample ;
A non-transitory computer-readable storage medium, wherein the MR information includes quantitative values of one or more MR parameters within voxels associated with the sample specified by the MR signal.
前記項が、前記測定デバイス内の前記コイルの前記コイル感度からの寄与を含む、請求項23に記載の非一時的なコンピュータ可読記憶媒体。 the nonlinear optimization problem includes a term corresponding to the square of the absolute value of the difference between the MR signal and the estimated MR signal corresponding to the MR information;
24. The non-transitory computer-readable storage medium of claim 23, wherein the term includes a contribution from the coil sensitivity of the coil within the measurement device.
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US201962907516P | 2019-09-27 | 2019-09-27 | |
US62/907,516 | 2019-09-27 | ||
PCT/US2020/052717 WO2021062154A1 (en) | 2019-09-27 | 2020-09-25 | Maxwell parallel imaging |
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JP2022548830A JP2022548830A (en) | 2022-11-22 |
JPWO2021062154A5 true JPWO2021062154A5 (en) | 2023-09-22 |
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US (1) | US11131735B2 (en) |
EP (1) | EP4034901A4 (en) |
JP (1) | JP2022548830A (en) |
KR (1) | KR102622283B1 (en) |
CN (1) | CN114450599B (en) |
BR (1) | BR112022004126A2 (en) |
CA (1) | CA3153503C (en) |
MX (1) | MX2022003462A (en) |
WO (1) | WO2021062154A1 (en) |
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2020
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