WO2008010221A1 - Method and system for signal processing - Google Patents

Method and system for signal processing Download PDF

Info

Publication number
WO2008010221A1
WO2008010221A1 PCT/IL2007/000901 IL2007000901W WO2008010221A1 WO 2008010221 A1 WO2008010221 A1 WO 2008010221A1 IL 2007000901 W IL2007000901 W IL 2007000901W WO 2008010221 A1 WO2008010221 A1 WO 2008010221A1
Authority
WO
WIPO (PCT)
Prior art keywords
signals
analog
signal
dimensional vector
analog signals
Prior art date
Application number
PCT/IL2007/000901
Other languages
French (fr)
Other versions
WO2008010221B1 (en
Inventor
Doron Kwiat
Original Assignee
Mri Microsystems Ltd.
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Mri Microsystems Ltd. filed Critical Mri Microsystems Ltd.
Publication of WO2008010221A1 publication Critical patent/WO2008010221A1/en
Publication of WO2008010221B1 publication Critical patent/WO2008010221B1/en

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/20Arrangements or instruments for measuring magnetic variables involving magnetic resonance
    • G01R33/28Details of apparatus provided for in groups G01R33/44 - G01R33/64
    • G01R33/32Excitation or detection systems, e.g. using radio frequency signals
    • G01R33/34Constructional details, e.g. resonators, specially adapted to MR
    • G01R33/341Constructional details, e.g. resonators, specially adapted to MR comprising surface coils
    • G01R33/3415Constructional details, e.g. resonators, specially adapted to MR comprising surface coils comprising arrays of sub-coils, i.e. phased-array coils with flexible receiver channels
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/20Arrangements or instruments for measuring magnetic variables involving magnetic resonance
    • G01R33/44Arrangements or instruments for measuring magnetic variables involving magnetic resonance using nuclear magnetic resonance [NMR]
    • G01R33/48NMR imaging systems
    • G01R33/54Signal processing systems, e.g. using pulse sequences ; Generation or control of pulse sequences; Operator console
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/20Arrangements or instruments for measuring magnetic variables involving magnetic resonance
    • G01R33/44Arrangements or instruments for measuring magnetic variables involving magnetic resonance using nuclear magnetic resonance [NMR]
    • G01R33/48NMR imaging systems
    • G01R33/54Signal processing systems, e.g. using pulse sequences ; Generation or control of pulse sequences; Operator console
    • G01R33/56Image enhancement or correction, e.g. subtraction or averaging techniques, e.g. improvement of signal-to-noise ratio and resolution
    • G01R33/5608Data processing and visualization specially adapted for MR, e.g. for feature analysis and pattern recognition on the basis of measured MR data, segmentation of measured MR data, edge contour detection on the basis of measured MR data, for enhancing measured MR data in terms of signal-to-noise ratio by means of noise filtering or apodization, for enhancing measured MR data in terms of resolution by means for deblurring, windowing, zero filling, or generation of gray-scaled images, colour-coded images or images displaying vectors instead of pixels

Landscapes

  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Signal Processing (AREA)
  • High Energy & Nuclear Physics (AREA)
  • Magnetic Resonance Imaging Apparatus (AREA)

Abstract

The invention provides a method and system for processing an n-dimensional vector of analog signals n analog signals (S1(t),…Sk(t),…Sn(t)). A non-singular linear transformation A is applied to the vector (S1(t),…Sk(t),…Sn(t)) to generate an n-dimensional vector of analog signals ( 1(t),… k(t),… n(t)). The analog signals 1(t) to n(t) are amplified to produce an n-dimensional vector of analog signals ( 1(t),… k(t),… n(t)).

Description

METHOD AND SYSTEM FOR SIGNAL PROCESSING
FIELD OF THE INVENTION
This invention relates to methods and systems for noise reduction in signals.
BACKGROUND OF THE INVENTION The present invention pertains to devices and systems generating a plurality of electronic signals. Such systems and devices typically include multiple detector arrays, such as are found in magnetic resonance imaging (MRI) devices, ultrasound imaging devices, and multiple antenna radar devices. These systems include one or more detectors that detect a time dependent level of a form of energy and generate an electronic signal correlative with the amount energy detected. The generated electronic signals contain noise arising from two sources. One source is random noise that was already present in the energy signal before being transduced into an electronic signal by a detector. Additional noise is subsequently introduced into the electronic signal by the electronics of the system. Methods are known for improving the signal to noise ratio in devices generating a plurality of electronic signals. One class of methods used to reduce noise attempts to decrease the noise in the energy signal by improving the conditions in which the energy signal is detected. For example, US Patent No. 7,187,169 discloses detecting nuclear magnetic resonance (NMR) signals in microtesla fields. Prepolarization in millitesla fields is followed by detection with an untuned dc superconducting quantum interference device (SQUID) magnetometer. Because the sensitivity of the SQUID is frequency independent, the signal-to-noise ratio (SNR) is enhanced by detecting the NMR signals in extremely low magnetic fields, where the NMR lines become very narrow even for grossly inhomogeneous measurement fields. This patent further discloses that an additional improvement of the signal to noise is obtained by use of a low noise polarization coil. US Patent 7,230,424 to Morrone discloses that phase shifting of the RF (radiofrequency) pulse used in MRI with each phase-encoding gradient level, improves the signal-to-noise ratio of the recorded signals by correcting for main magnetic field inhomogeneities. Other methods for noise reduction attempt to remove noise from the electronic signals by mathematically processing the signals. US Patent No. 6,992,484 to Frank, for example discloses a method for analyzing MRI diffusion data in which methods of mathematical group theory are used to reduce noise in the signals. US Patent No. 6,486,671 discloses improvement of MRI image quality using matrix regularization. A correction matrix is defined that is used to alter the sensitivities matrix and the altered sensitivities matrix and the intensity matrix are used to generate an estimated spin density matrix which is used to generate the final image.
SUMMARY OF THE INVENTION
The present invention provides a method for processing a plurality of analog signals. The analog signals may be, for example, analog signals produced by a multi- detector device, such as an MRI system ultrasound imaging devices, and multiple antenna radar devices. As further examples, the analog signals may be seismographic signals, RGB encoding and decoding signals, sound signals and astronomical signals.
The system and method of the invention receives as an input n analog signals S1Ct) to Sn(t) having about the same signal to noise ratio that are input to an analog signal adder. The analog signal adder outputs n analog signals σ^t) to σπ(t), where each of the analog signals σ^t) to σn(t) is a linear combination of the n input signals Si(t) to Sn(t). The ή-dimensional vector of signals (σi(t),...σj(t),...σn(t)) is thus obtained by applying a linear transformation A to the n-dimensional input vector of signals (S1(t)...Sj(t)...Sn(t)).
The analog signals σι (t) to σn(t) are amplified using one or more analog signal amplifiers. If the input signals S1(I) to Sn(t) are uncorrelated and have about the same signal-to-noise ratio, the signals σ^t) to σn(t), being a linear combination of the signals Si(t) to Sn(t), will have a lower signal-to-noise ratio than that of the signals Si(t) to Sn(t). The signal-to-noise ratio of a signal θj(t) will be reduced from that of the input signals by a factor of 1/ Λ[N , where N is the number of input signals of which σj(t) is a linear combination. Thus, the larger N, the lower the signal-to-noise ratio of the σj(t). Since the signals σ1(t),...σic(t),...σn(t) have a higher signal to noise ratio than the signals S1(I) to Sn(t), the amplification may be accomplished using amplifier or amplifiers having a lower sensitivity than would be required to amplify the signals Si(t) to Sn(t). The amplified signals are digitized. A'1 (the inverse of the linear transformation
A) is applied to the vector of the digitized signals to generate digital signals S'^tj) to S'n(tj), which is the output of the method and system of the invention.
It will also be understood that the system according to the invention may be a suitably programmed computer. Likewise, the invention contemplates a computer program being readable by a computer for executing the method of the invention. The invention further contemplates a machine-readable memory tangibly embodying a program of instructions executable by the machine for executing the method of the invention.
Thus, in its first aspect, the invention provides a method for processing an n- dimensional vector of analog signals n analog signals (S1(I),...Sk(t),...Sn(t)) comprising:
(a) applying a non-singular linear transformation A to the vector (Si(t),...Sk(t),...Sn(t)) to generate an n-dimensional vector of analog signals (σj(t),...σk(t),...σn(t)); and
(b) amplifying each of the analog signals σ^t) to σn(t) to produce an n-dimensional vector of analog signals (∑!(t), ... Σ k(t), ... ∑n(t))-
In its second aspect, the invention provides a system for processing an n- dimensional vector of analog signals n analog signals (Si(t),...Sk(t),...Sn(t)) comprising:
(a) an analog signal adder applying a non-singular linear transformation A to the vector (S1(I)5...Sk(t),...Sn(t)) to generate an n-dimensional vector of analog signals
1(t),...σk(t),...σn(t)); and
(b) one or more analog signal amplifiers amplifying the analog signals σ^t) to σn(t) to produce an n-dimensional vector of analog signals (∑i(t),...Σ k(t),...∑n(t)). BRIEF DESCRIPTION OF THE DRAWING
In order to understand the invention and to see how it may be carried out in practice, embodiments will now be described, by way of non-limiting example only, with reference to the accompanying drawings, in which: Fig. 1 shows a system for processing signals generated by a multi-detector device, in accordance with one embodiment of the invention; and
Fig. 2 shows a magnet.
DETAILED DESCRIPTION OF EMBODIMENTS
Fig. 1 shows schematically a system 2 for processing a plurality of signals. The system 2 receives as an input n analog signals S1(O to Sn(t) having similar signal to noise ratios and outputs n digital signals S'i(t,) to S'n(tj). The n analog signals S1(O to
Sn(t) are input to an analog signal adder 4. The analog signal adder 4 outputs n analog signals σ^t) to σn(t), where each of the analog signals σi(t) to σn(t) is a linear combination of the n input signals S1(O to Sn(t). The signals σ^t) to σn(t), being a linear combination of the signals S1(Q to Sn(O, will have a higher signal to noise ratio than the signals Si(t) to Sn(t). The n-dimensional vector of input signals (Si(t),...Sk(t),...Sn(t)) can thus be related to the n-dimensional output vector of the adder 4
(σi(t),...σk(t),...σn(t)) by
ntf SKt)
Figure imgf000005_0001
where A is a non-singular nXn matrix.
In a preferred embodiment of the invention, the entries of the matrix A are selected from -1, 0 and 1. In a more preferred embodiment, the entries of the matrix A are selected from 0 and 1. In another preferred embodiment, each row of the matrix A contains exactly 1 0. In this case, each of the signals σ^t) to σn(t) is a linear combination of a unique combination of n-1 of the n signals S1(O to Sn(t).
The analog signal adder 4 may be implemented by permanent electrical connections between the input signals Si(t) to Sn(t). Alternatively, the adder 4 may be implemented by temporarily electrical connections between the input signals by means of switching devices. Alternatively, the adder 4 maybe implemented by multiple encoding of the input signals, so that all of the input signals having a particular code are summed together. The multiple encoding may be, for example, frequency encoding,as disclosed in PCT.
Each of the signals σ1(t),...σic(t),...σn(t) is amplified by means of an analog signal amplifier 6. Each of the n signals σi(t),...σk(t),...σn(t) may be amplified by a separate amplifier 6, as shown in Fig. 1. Alternatively, a single amplifier 6 may be used, where amplification of the signals σ1(t),...σic(t),...σn(t) occurs via multiplexing of the n signals through a common amplifier 6 (not shown). Since the signals σ1(t),...σk(t),...σn(t) have a higher signal to noise ratio than the signals S1Ct) to Sn(t), amplifier or amplifiers 6 may be used having a lower sensitivity than would be required to amplify the signals S1Ct) to Sn(t).
The result of the amplification is an n-dimensional vector of amplified analog signals ∑i(t),...∑k(t),...∑n(t). Each of the amplified signals ∑1(t),...∑k(t),...∑n(t) is converted to a digital signal ∑'i(tj),...Σ'kOj),.. -∑'nOj), respectively, by means of an analog to digital converter 8. Each of the n analog signals ∑i(t),...∑k(t),...∑n(t) may be digitized by a separate analog to digital converter 8, as shown in Fig. 1. Alternatively, a single analog to digital converter 8 may be used, where amplification of the signals Σ j (t), ... ∑k(t), ... ∑n(t) occurs via multiplexing of the n signals through a common analog to digital converter 8 (not shown). The multiplexing may be time multiplexing or may coding multiplexing in which each of the signals ∑1(t),...∑k(t),...∑n(t) is, for example, frequency encoded as disclosed in PCT....
The n-dimensional vector of digital signals ∑'1(t),...∑'k(t),...∑'n(t). is input to a digital signal adder 10. The digital signal adder 10 is a signal processing module that executes a signal recovery algorithm which generates the n digital signals S'i(t) to S'n(t) from the n digital signals ∑'1(t),...∑'k(t),...∑'n(t). The signal vector ∑'i(t),...∑lk(t),...∑f n(t) that is input to the digital signal adder 10 is multiplied by the matrix A"1, where A"1 is the inverse of the matrix A:
Figure imgf000007_0001
Example In an implementation of the invention for the processing of 9 signals, the 9X9 non-singular matrix A may be used, where
In the matrix A, the entry
Figure imgf000007_0002
if the input signal Sj(t) is not. a component of σj(t). Thus, for example, σ1(t)=S1(t)+ S2(t)+ S3(t)+ S8(t) and σ2(t)=S4(t)+ S5(t)+ S6(t). The signal-to-noise ratio of σi(t) would be about equal to l/V-4 = 0.5 times that of the input signals, while the signal-to-noise ratio of σ2(t) would be about equal to 1/ -Jϊ = 0.58 times that of the input signals.
A" is given by: 0.57 0.29 0.14 0.14 0.86 0.57 0.57 0.29 0.14
1.14 1.57 1.29 1.29 1.71 1.14 0.14 0.43 0.29
0.57 0.29 0.14 0.14 0/14 0.43 0.43 0.71 0.14
0.29 0.14 0.57 0.57 0.43 0.29 0.29 0.14 0.57
A = 0.14 0.57 0.29 0.29 0.29 0.14 0.14 0.57 0.29
0.14 0.57 0.29 0.29 0.71 0.14 0.14 0.57 0.29
0.29 0.14 0.43 0.57 0.43 0.29 0.29 0.14 0.43
1.00 1.00 1.00 1.00 1.00 1.00 0.00 0.00 0.00
0.71 0.86 0.43 0.43 0.57 0.71 0.29 0.14 0.43
The invention also provides a method to produce a magnet. A U-shaped magnet may be made by combining pre-magnetized NdFeB sectors and assembling them piecewise in such manner that all North poles are pointing in parallel and thus a collection of such small magnets creates a larger magnet of a desired arc length and thickness. (See Fig. 2).
Another method of manufacturing a U-shaped magnet is to first assemble unmagnetized bricks of NdFeB sectors into a large U-shape of a desired shape and size. One then attaches a mirror U-shape solenois without an iron core.
Once attached to the NdFeB U-shape, a signiiicanlyt large current pulse is passed through the coil, thus creating a magnetic field strong enough to have the NdFeB U-shape magnetized in the desired direction.

Claims

CLAIMS:
1. A method for processing an n-dimensional vector of analog signals n analog signals (S1(t),...Sk(t),...Sn(t)) comprising:
(a) applying a non-singular linear transformation A to the vector (S1(Q5... Sk(t),...Sn(t)) to generate an n-dimensional vector of analog signals (σ1(t)5...σk(t),...σn(t)); and
(b) amplifying each of the analog signals σi(t) to σn(t) to produce an n-dimensional vector of analog signals (∑i(t),...Σ k(t),...∑n(t)).
2. The method according to Claim 1 further comprising: (a) digitizing the analog signals ∑'i(t) to ∑'n(t) to produce an n- dimensional vector of digital signals (∑'i(t),...∑liζ(t),...∑'n(t)); and (b) applying to the n-dimensional vector of digital signals
(∑'i (t), ... ∑'k(t), .. • ∑'n(t)) the linear transformation A"1.
3. The method according to Claim 1 or 2 wherein the signals S1(O to Sn(t) have about the same signal to noise ratio.
4. The method according to any one of the previous claims wherein the signals S i (t), ... Sk(t), ... Sn(t) are uncorrelated.
5. The method according to Claim 1 wherein the step of amplifying each of the analog signals σi(t) to σn(t) is accomplished using a separate analog signal amplifier for each signal.
6. The method according to Claim 1 wherein the step of amplifying each of the analog signals σ^t) to σn(t) is accomplished using a single analog signal amplifier and multiplexing the signals to the amplifier.
7. The method according to Claim 6 wherein the multiplexing is time multiplexing.
8. The method according to Claim 6 wherein the multiplexing is signal encoded multiplexing.
9. The method according to Claim 8 wherein the signal encoding is frequency encoding.
10. The method according to any one of the previous claims wherein the signals Si(t) to Sπ(t) are MRI signals.
11. The method according to any one of the previous claims wherein all entries of the matrix A are selected from -1, 0, and 1.
12. The method according to Claiml 1 wherein all entries of the matrix A are selected from 0, and 1.
5 13. The method according to any one of the previous claims wherein the matrix A has exactly one 0 in each row.
14. A system for processing an n-dimensional vector of analog signals n analog signals (S1(Q5... Sk(t),... Sn(O) comprising:
(a) an analog signal adder applying a non-singular linear 10 transformation A to the vector (S i(t), ... Sk(t), ... Sn(O) to generate an n-dimensional vector of analog signals (σi(t)5...σk(t)5...σn(t)); and
(b) one or more analog signal amplifiers amplifying the analog signals σi(t) to σn(t) to produce an n-dimensional vector of
15 analog signals (E1(O,...Σ k(t),...∑n(t)).
15. The system according to Claim 1 further comprising:
(a) one or more analog to signal converters digitizing the analog signals ∑'^t) to ∑'n(t) to produce an n-dimensional vector of digital signals (∑l 1(t),...∑l k(t),...∑f n(t)); and
20 (b) a digital signal adder applying to the n-dimensional vector of digital signals (∑'i(t),...∑'k(t),...∑'n(t)) the linear transformation A"1.
16. The system according to Claim 14 or 15 wherein the signals S1(O to Sn(t) have about the same signal to noise ratio.
25 17. The system according to any one of Claims 14 to 16 wherein the signals
S i (t), ... Sk(t), ... Sn(O are uncorrelated.
18. The system according to Claim 14 comprising a separate analog signal amplifier for each signal, each analog signal amplifier amplifying a different one of the analog signals σi(t) to σn(t). 30
19. The system according to Claim 14 comprising a single analog signal amplifier and a multiplexer multiplexing the signals σj(t) to σn(t) to the amplifier.
20. The system according to Claim 19 wherein the multiplexing is time multiplexing.
21. The system according to Claim 19 wherein the multiplexing is signal encoded multiplexing.
5 22. The system according to Claim 21 wherein the signal encoding is frequency encoding.
23. The system according to any one of Claimsl4 to 22 wherein the signals S1(Q to Sn(t) are MRI signals.
24. The system according to any one of Claims 14 to 23 wherein all entries of the 10 matrix A are selected from —1, 0, and 1.
25. The system according to Claim24 wherein all entries of the matrix A are selected from 0, and 1.
26. The system according to any one of Claims 14 to 25 wherein the matrix A has exactly one 0 in each row.
15 27. A computer program comprising computer program code means for performing all the steps of Claim 1 when said program is run on a computer.
28. A computer program as claimed in Claim 28 embodied on a computer readable medium.
PCT/IL2007/000901 2006-07-17 2007-07-17 Method and system for signal processing WO2008010221A1 (en)

Applications Claiming Priority (2)

Application Number Priority Date Filing Date Title
IL176906A IL176906A0 (en) 2006-07-17 2006-07-17 Deterministic detection of signals in a detector array
IL176906 2006-07-17

Publications (2)

Publication Number Publication Date
WO2008010221A1 true WO2008010221A1 (en) 2008-01-24
WO2008010221B1 WO2008010221B1 (en) 2008-03-06

Family

ID=38566954

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/IL2007/000901 WO2008010221A1 (en) 2006-07-17 2007-07-17 Method and system for signal processing

Country Status (2)

Country Link
IL (1) IL176906A0 (en)
WO (1) WO2008010221A1 (en)

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2003003037A2 (en) * 2001-06-18 2003-01-09 Mri Devices Corporation Method and apparatus for enhanced multiple coil mr imaging
WO2003021859A1 (en) * 2001-08-31 2003-03-13 Broadband Physics, Inc. Compensation for non-linear distortion in a modem receiver
US20030062894A1 (en) * 2001-10-01 2003-04-03 Siemens Aktiengesellschaft Magnetic resonance signal evaluation method and apparatus using combinations of simultaneously received antenna signals
US20030214299A1 (en) * 2002-05-17 2003-11-20 General Electric Company RF detector array for magnetic resonance imaging

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2003003037A2 (en) * 2001-06-18 2003-01-09 Mri Devices Corporation Method and apparatus for enhanced multiple coil mr imaging
WO2003021859A1 (en) * 2001-08-31 2003-03-13 Broadband Physics, Inc. Compensation for non-linear distortion in a modem receiver
US20030062894A1 (en) * 2001-10-01 2003-04-03 Siemens Aktiengesellschaft Magnetic resonance signal evaluation method and apparatus using combinations of simultaneously received antenna signals
US20030214299A1 (en) * 2002-05-17 2003-11-20 General Electric Company RF detector array for magnetic resonance imaging

Non-Patent Citations (3)

* Cited by examiner, † Cited by third party
Title
A.REYKOWSKI ET AL.: "Mode Matrix - A Generalized Signal Combiner For Parallel Imaging Arrays", PROC.INTL.SOC.MAG.RESON.MED. 11, 2004, pages 1587, XP002455190 *
KWIAT D ET AL: "A DECOUPLED COIL DETECTOR ARRAY FOR FAST IMAGE ACQUISITION IN MAGNETIC RESONANCE IMAGING", MEDICAL PHYSICS, AIP, MELVILLE, NY, US, vol. 18, no. 2, 1 March 1991 (1991-03-01), pages 251 - 265, XP000228811, ISSN: 0094-2405 *
STEYSKAL H ET AL: "Mutual coupling compensation in small array antennas", IEEE TRANSACTIONS ON ANTENNAS AND PROPAGATION, IEEE SERVICE CENTER, PISCATAWAY, NJ, US, vol. 38, no. 12, December 1990 (1990-12-01), pages 1971 - 1975, XP002155205, ISSN: 0018-926X *

Also Published As

Publication number Publication date
IL176906A0 (en) 2007-05-15
WO2008010221B1 (en) 2008-03-06

Similar Documents

Publication Publication Date Title
US7005853B2 (en) Prior-information-enhanced dynamic magnetic resonance imaging
US6377044B1 (en) Multi-mode receiver coils for MRI
US10274566B2 (en) Dixon-type water/fat separation MRI using high-SNR in-phase image and lower-SNR at least partially out-of-phase image
US11275135B2 (en) Method and device for taking account of the magnetic resonance signal during interference suppression
JP5260819B2 (en) Method and system for speeding up imaging using parallel MRI
US10114096B2 (en) Multi-slice magnetic resonance data acquisition method and imaging apparatus
US6914432B2 (en) Phased array coil assembly and method and system for employing the same
WO2011087847A2 (en) Accelerated mri with nonlineear spatial encoding gradients
JP6074126B1 (en) Zero echo time MR imaging using sampling in the center of k-space
US20050174113A1 (en) Magnetic resonance imaging method with accelerated data acquisition
US10895619B2 (en) MR imaging with Dixon-type water/fat separation
US20210109181A1 (en) Mr imaging using a stack-of-stars acquisition with intrinsic motion correction
WO2008010221A1 (en) Method and system for signal processing
JPH04246327A (en) Dynamic mr imaging method
US20200217909A1 (en) System and method for increased signal-to-noise ratio in multi spin-echo pulse imaging
US9030338B2 (en) EMI reduction with specific coding of counter signals
Oh et al. Dynamic range expansion of receiver by using optimized gain adjustment for high‐field MRI
KR101330945B1 (en) Epi image correction method and epi image correction system thereof
Bain Heteronuclear chemical-shift correlation by fully coupled phase-sensitive two-dimensional NMR, a robust experiment
EP4012434A1 (en) Dixon-type water/fat separation mr imaging
JPS62246355A (en) Magnetic resonance imaging apparatus
JPH06169897A (en) Magnetic resonance imaging system
Clarke et al. NMR and MRI apparatus and method
WO2023025614A1 (en) Coherence filtering for magnetic resonance imaging (mri) signals
JPH04246326A (en) Mr imaging method

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: 07789956

Country of ref document: EP

Kind code of ref document: A1

NENP Non-entry into the national phase

Ref country code: DE

NENP Non-entry into the national phase

Ref country code: RU

32PN Ep: public notification in the ep bulletin as address of the adressee cannot be established

Free format text: F1205A "NOTING OF LOSS OF RIGHTS PURSUANT TO RULE 112(1) EPC"

122 Ep: pct application non-entry in european phase

Ref document number: 07789956

Country of ref document: EP

Kind code of ref document: A1