IP Library Granted Patent US 12,332,331
Granted Patent B2
US 12,332,331 · App. 17/905,716 · Granted Jun 17, 2025

Pulse sequences and frequency sweep pulses for single-sided magnetic resonance imaging

Inventors: Muller Francis De Matos Gomes (Hayward, CA); Aleksandar Nacev (San Francisco, CA)
Assignee: Promaxo, Inc.
G01R33/3607A61B5/055G01R33/445G01R33/3802G01R33/3808G01R33/483
View Patent ↗
Loading inventors, assignments & file history…
Monitor This Case
Get email alerts when status or documents change.
Order Certified Copies
Most orders are placed with the USPTO same day — all within 24 business hours.
Order via The Patent Place →
Pre-filled with this patent's details
Quick Facts
Patent No.
US 12,332,331
App. No.
17/905,716
Granted
Jun 17, 2025
Kind
B2
Abstract

Single-sided MRI scanners, systems, and methods are disclosed. A method can include applying a first sweeping frequency pulse defining an X axis; applying a second sweeping frequency pulse defining a Y axis; applying a third sweeping frequency pulse defining the Y axis; and applying a fourth sweeping frequency pulse defines a −X axis. The sweep rate of the fourth sweeping frequency pulse can be less than the sweep rate of the third and/or second sweeping frequency pulse. The sweeping frequency pulses can be chirp pulses. Frequency sweep DEFT pulse sequences can provide the benefits of a broader bandwidth and less sensitivity to the inhomogeneity of a single-sided MRI scanner.

Claims (36)

1. A method for transmitting radio frequency pulses for a single-sided magnetic imaging apparatus, wherein an inherent gradient magnetic field extends from the magnetic imaging apparatus relative to a first axis into the field of view, and wherein the method comprises:

applying a first sweeping frequency pulse having a first duration and a first sweep rate, wherein the first sweeping frequency pulse defines an X axis, wherein the first sweeping frequency pulse comprises a first 90 degree pulse configured to rotate the magnetization to a transverse plane for the first duration;

applying a second sweeping frequency pulse having a second duration and a second sweep rate, wherein the second sweeping frequency pulse defines a first Y axis;

applying a third sweeping frequency pulse having a third duration and a third sweep rate, wherein the third sweeping frequency pulse defines a second Y axis; and

applying a fourth sweeping frequency pulse having a fourth duration and a fourth sweep rate, wherein the fourth sweeping frequency pulse defines a −X axis, wherein the fourth sweeping frequency pulse comprises a second 90 degree pulse configured to rotate the magnetization back to the first axis, and wherein the fourth sweep rate is less than the third sweep rate.

2. The method of claim 1 , wherein the second sweeping frequency pulse comprises a first 180 degree pulse configured to invert the magnetization to rewind any phase accumulated during the time it spends in the transverse plane, and wherein the third sweeping frequency pulse comprises a second 180 degree pulse configured to invert the magnetization to rewind any phase accumulated during the time it spends in the transverse plane.

3. The method of claim 1 , wherein the sweep rates comprise linear rates.

4. The method of claim 1 , wherein the fourth sweep rate is half the third sweep rate.

5. The method of claim 1 , wherein the sweep rate of each pulse is constant.

6. The method of claim 1 , wherein the first sweep rate is fixed and increases the frequency of the radio frequency pulse from negative to positive.

7. The method of claim 1 , wherein at least two of the first duration, the second duration, the third duration, and the fourth duration are the same.

8. The method of claim 1 , wherein at least two of the first sweep rate, the second sweep rate, third sweep rate, and the fourth sweep rate are the same.

9. The method of claim 1 , wherein the first sweeping frequency pulse comprises a first excitation pulse, wherein the second sweeping frequency pulse comprises a first refocusing pulse, wherein the third sweeping frequency pulse comprises a second refocusing pulse, and wherein the fourth sweeping frequency pulse comprises a second excitation pulse.

10. The method of claim 1 , wherein the first frequency sweeping pulse, the second frequency sweeping pulse, the third frequency sweeping pulse, and the fourth frequency sweeping pulse define a frequency of between 1 Megahertz and 21 Megahertz.

11. The method of claim 1 , wherein the magnetic field strength in the field of view is less than 1 Tesla, and wherein the inhomogeneity of the magnetic field is between 200 ppm and 200,000 parts per million.

12. A magnetic imaging apparatus, comprising:

a permanent magnet comprising a face;

a gradient coil set;

an electromagnet;

a radio frequency coil, wherein an inherent gradient magnetic field extends from the magnetic imaging apparatus relative to a first axis into the field of view, wherein the first axis is perpendicular to the face of the permanent magnet; and

a control circuit configured to control the radio frequency coil to:

apply a first sweeping frequency pulse having a first duration and a first sweep rate, wherein the first sweeping frequency pulse defines a second axis that is orthogonal to the first axis, wherein the first sweeping frequency pulse comprises a 90 degree pulse configured to rotate the magnetization to a transverse plane for the first duration;

apply a second sweeping frequency pulse having a second duration and a second sweep rate, wherein the second sweeping frequency pulse defines a third axis that is orthogonal to the first axis and to the second axis;

apply a third sweeping frequency pulse having a third duration and a third sweep rate, wherein the third sweeping frequency pulse defines the third axis; and

apply a fourth sweeping frequency pulse having a fourth duration and a fourth sweep rate, wherein the fourth sweeping frequency pulse defines the negative second axis, wherein the fourth sweeping frequency pulse comprises a second 90 degree pulse configured to rotate the magnetization back to the first axis, and wherein the fourth sweep rate is less than the third sweep rate.

13. The magnetic imaging apparatus of claim 12 , wherein the second sweeping frequency pulse comprises a first 180 degree pulse configured to invert the magnetization to rewind any accumulated phase, and wherein the third sweeping frequency pulse comprises a second 180 degree pulse configured to invert the magnetization to rewind any accumulated phase.

14. The magnetic imaging apparatus of claim 12 , wherein the first sweeping frequency pulse defines an X axis, wherein the second sweeping frequency pulse and the third sweeping frequency pulse define a Y axis, and wherein the fourth sweeping frequency pulse defines a −X axis.

15. The magnetic imaging apparatus of claim 12 , wherein the fourth sweep rate is half the third sweep rate.

16. The magnetic imaging apparatus of claim 12 , wherein the sweep rates are constant throughout each pulse.

17. The magnetic imaging apparatus of claim 16 , wherein the first frequency sweep rate increases the frequency from high to low.

18. The magnetic imaging apparatus of claim 12 , wherein at least two of the first duration, the second duration, the third duration, and the fourth duration are the same.

19. The magnetic imaging apparatus of claim 12 , wherein at least two of the first sweep rate, the second sweep rate, third sweep rate, and the fourth sweep rate are the same.

20. The magnetic imaging apparatus of claim 12 , wherein the first sweeping frequency pulse comprises a first excitation pulse, wherein the second sweeping frequency pulse comprises a first refocusing pulse, wherein the third sweeping frequency pulse comprises a second refocusing pulse, and wherein the fourth sweeping frequency pulse comprises a second excitation pulse.

21. The magnetic imaging apparatus of claim 12 , wherein the radio frequency coil is configured to transmit pulses having a frequency between 1 Megahertz and 21 Megahertz.

22. The magnetic imaging apparatus of claim 12 , wherein the magnetic field strength in the field of view is less than 1 Tesla, and wherein the inhomogeneity of the magnetic field is between 200 ppm and 200,000 ppm.

23. The magnetic imaging apparatus of claim 12 , wherein the radio frequency coil comprises a radio frequency transmission coil and a radio frequency reception coil.

Assignments (4)
INTELLECTUAL PROPERTY SECURITY AGREEMENT Recorded Jul 2, 2026
From: PROMAXO LLC
To: WINDWARD FAMILY OFFICE, LLC
Reel/Frame 075893/0395 →
SECURITY INTEREST Recorded Sep 17, 2025
From: PROMAXO LLC
To: EASTWARD FUND MANAGEMENT, LLC
Reel/Frame 072916/0001 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 15, 2025
From: NACEV, ALEKSANDAR; DE MATOS GOMES, MULLER FRANCIS
To: PROMAXO, INC.
Reel/Frame 071128/0431 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Sep 6, 2022
From: NACEV, ALEKSANDAR; GOMES, MULLER
To: PROMAXO, INC.
Reel/Frame 060999/0092 →
Continuity (2)
Provisional Application 62987286 · Mar 9, 2020
Related Publication 20230296707A1 · Sep 21, 2023
References Cited (46)
US 4801884A · Oppelt et al. · 1989 [cited by applicant]
US 4893081A · Zur · 1990 [cited by applicant]
US 5303705A · Nenov · 1994 [cited by applicant]
US 5320099A · Roberts et al. · 1994 [cited by applicant]
US 5448170A · Bodenhausen et al. · 1995 [cited by applicant]
US 6054853A · Miyamoto et al. · 2000 [cited by applicant]
US 9513358B2 · Levin · 2016 [cited by examiner]
US 10234524B2 · Zeller · 2019 [cited by examiner]
US D895803S · Nacev et al. · 2020 [cited by applicant]
US D942012S · Nacev et al. · 2022 [cited by applicant]
US 11506737B2 · Gomes · 2022 [cited by applicant]
US D980981S · Nacev et al. · 2023 [cited by applicant]
US 11609291B2 · Nacev et al. · 2023 [cited by applicant]
US 11656303B2 · Nacev et al. · 2023 [cited by applicant]
US 11921178B2 · De Matos Gomes · 2024 [cited by applicant]
US 20180356480A1 · Weinberg et al. · 2018 [cited by applicant]
US 20220113361A1 · Nacev et al. · 2022 [cited by applicant]
US 20220146613A1 · Gomes · 2022 [cited by applicant]
US 20220342020A1 · Narayanan et al. · 2022 [cited by applicant]
US 20230104153A1 · Gomes et al. · 2023 [cited by applicant]
US 20230106912A1 · Kumar et al. · 2023 [cited by applicant]
US 20230109705A1 · De Matos Gomes · 2023 [cited by applicant]
US 20230110217A1 · Nacev et al. · 2023 [cited by applicant]
CN 103976735A · 2014 [cited by applicant]
JP H05507210A · 1993 [cited by applicant]
JP 2004166751A · 2004 [cited by applicant]
JP 2004313276A · 2004 [cited by applicant]
WO 2014203253A1 · 2014 [cited by applicant]
WO WO2020168233A1 · 2020 [cited by applicant]
WO WO2020172672A1 · 2020 [cited by applicant]
WO WO2020172673A1 · 2020 [cited by applicant]
WO WO2020198395A1 · 2020 [cited by applicant]
WO WO2020198396A1 · 2020 [cited by applicant]
WO WO2020264194A1 · 2020 [cited by applicant]
WO WO2021150902A1 · 2021 [cited by applicant]
WO WO2021168291A2 · 2021 [cited by applicant]
WO 2021183482A1 · 2021 [cited by applicant]
WO WO2021183484A1 · 2021 [cited by applicant]
International Search Report and Written Opinion for International PCT Application No. PCT/US2021/021461, dated Jun. 14, 2021. [cited by applicant]
Stockman et al., Transmit Array Spatial Encording (TRASE) using broadband WURST pulses for RF spatial encoding in inhomogeneous Bo fields, Journal of Magnetic Resonance (Apr. 8, 2016), 268:36-48. [cited by applicant]
Cooley et al., Two-Dimensional Imaging in a Lightweight Portable MRI Scanner without Gradient Coils, Magnetic Resonance in Medicine (2015), 73:872-883. [cited by applicant]
Dumez et al., Multidimensional excitation pulses based on spatiotemporal encoding concepts, Journal of Magnetic Resonance (Nov. 7, 2012), 226:22-34. [cited by applicant]
Tal et al., Spatial encoding and the single-scan acquisition of high definition MR images in inhomogeneous fields, Journal of Magnetic Resonance (Jul. 14, 2006), 182:179-194. [cited by applicant]
JP Serial No. 2022-554409 Office Action dated Sep. 3, 2024. [cited by applicant]
PCT/US2021/021461 International Preliminary Report on Patentability dated Sep. 6, 2022. [cited by applicant]
JP2022-554409 Office Action dated Apr. 10, 2025, and an English translation. [cited by applicant]