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    • 24. 发明授权
    • Magnetic field dosimeter
    • 磁场剂量计
    • US07936168B2
    • 2011-05-03
    • US11663825
    • 2005-09-28
    • Stuart CrozierStephen James WilsonIan Gregg
    • Stuart CrozierStephen James WilsonIan Gregg
    • G01R33/02G01R33/07
    • G01D9/005G01R33/02G01R33/022
    • A portable device is used to measure exposure to magnetic fields and/or exposure to changes of magnetic field. The device (10) includes a first sensor (14) for measuring instantaneous magnetic field strength, and a second sensor (15) which is located adjacent to, and orientated in the same direction as, the first sensor for providing an output indicative of the time rate of change of the magnetic field. An integrator (22) integrates the rate of change output from the second sensor (15) over time to derive relative changes in the magnetic field. A processor (20) is connected to the outputs of at least the first sensor and the integrator. The processor selectively provides an indication of field strength from the output of the first sensor if the output is within the normal operating range of the first sensor, or otherwise from the integrator. A memory (24) is connected to the output of the second sensor (15) to store cumulative exposure to changes in the magnetic field. Three pairs of first and second sensors may be orientated in respective orthogonal directions.
    • 便携式设备用于测量磁场的暴露和/或暴露于磁场的变化。 装置(10)包括用于测量瞬时磁场强度的第一传感器(14)和与第一传感器相邻并定向于与第一传感器相同方向定位的第二传感器(15),用于提供指示 磁场的时间变化率。 积分器(22)将随着时间推移从第二传感器(15)输出的变化率积分以导出磁场的相对变化。 处理器(20)至少连接到第一传感器和积分器的输出。 如果输出在第一传感器的正常操作范围内,或者来自积分器,则处理器选择性地从第一传感器的输出提供场强的指示。 存储器(24)连接到第二传感器(15)的输出端以存储对磁场变化的累积曝光。 可以在各个正交方向上定向三对第一和第二传感器。
    • 27. 发明授权
    • Magnets for use in magnetic resonance imaging
    • 用于磁共振成像的磁铁
    • US08421463B2
    • 2013-04-16
    • US12447070
    • 2007-10-26
    • Stuart CrozierHuawei ZhaoFeng Liu
    • Stuart CrozierHuawei ZhaoFeng Liu
    • G01V3/00
    • G01R33/3815G01R33/421
    • A magnetic resonance system uses a shielded superconducting magnet to produce a dsv useful for specialist imaging in an overall short magnet system at field strengths 1.5 Tesla and above. The magnet includes at least a first central coil C1, which has a length of at least 25% of the overall length of the magnet, and is used in concert with a series of symmetric primary coils, at least one set of which carry current in a direction opposite to that of the central coil. Force balancing is advantageously used in the design of the coils. The primary coils are shielded by at least one shielding coil, which carries current in a direction opposite to the majority of the primary coils. The magnet resonance system can be used for orthopedic imaging.
    • 磁共振系统使用屏蔽超导磁体产生一个dsv,用于整个短磁体系统中的专家成像,场强为1.5特斯拉及以上。 该磁体包括至少一个第一中心线圈C1,该中心线圈C1的长度至少为磁铁整体长度的25%,并与一系列对称的初级线圈一致使用,至少一组载体电流 与中心线圈相反的方向。 力平衡有利地用于线圈的设计中。 初级线圈由至少一个屏蔽线圈屏蔽,该屏蔽线圈沿与大部分初级线圈相反的方向承载电流。 磁共振系统可用于矫形成像。
    • 28. 发明申请
    • OPEN-BORE MAGNET FOR USE IN MAGNETIC RESONANCE IMAGING
    • 用于磁共振成像的开放磁体
    • US20120258862A1
    • 2012-10-11
    • US13518117
    • 2010-12-20
    • Feng LiuRiyu WeiStuart Crozier
    • Feng LiuRiyu WeiStuart Crozier
    • G01R33/3815G01R33/035
    • G01R33/3815H01F6/06
    • A magnetic resonance system is provided which employs a shielded, electromagnetically asymmetric and low-stress magnet to produce a superior sized imaging region close to the patient side. The magnet has a double layered configuration. In the primary layer, the magnet includes at least two strongest coils at two ends of the magnet (end coils), which carry current in the same direction. The magnet may include at least one coil close to the end coils which carries current in a direction opposite to that of the end coils. The magnet employs a plurality of smaller sized coils (4-7, relative to the large end-coils) in the central region of the primary layer, and these coils are located asymmetrically relative to the imaging region centre. The magnet is shielded by a plurality (1-5) of shielding coils, which carry current in a direction opposite to that of the end-coils at primary layer. Compared with conventional short-bore magnets, the magnet of the invention offers an accessible imaging region with significantly enlarged imaging region, and it can be used in, for example, body-part or whole-body imaging.
    • 提供一种磁共振系统,其采用屏蔽的电磁不对称和低应力磁体来产生靠近患者侧的高级成像区域。 磁体具有双层结构。 在主层中,磁体包括在磁体(端部线圈)的两端处的至少两个最强的线圈,其在同一方向上承载电流。 磁体可以包括靠近端部线圈的至少一个线圈,其在与端部线圈的方向相反的方向上承载电流。 磁体在主层的中心区域使用多个较小尺寸的线圈(相对于大端部线圈的4-7),并且这些线圈相对于成像区域中心不对称地定位。 磁体被多个(1-5)的屏蔽线圈屏蔽,该屏蔽线圈在主层上沿着与末端线圈相反的方向承载电流。 与传统的短孔磁体相比,本发明的磁体提供了一种具有显着放大的成像区域的可访问成像区域,并且可以用于例如身体部位或全身成像。
    • 29. 发明申请
    • COIL DECOUPLING
    • 线圈解锁
    • US20100182009A1
    • 2010-07-22
    • US12593237
    • 2008-03-26
    • Stuart CrozierBing Keong LiEwald Weber
    • Stuart CrozierBing Keong LiEwald Weber
    • G01R33/36
    • G01R33/34046A61B5/055G01R33/34076G01R33/365G01R33/5611
    • A Magnetic Resonance Imaging (MRI) phased array head coil (10) comprises an array of coils (1, 2, 3, 4) a decoupling circuit (7) and a decoupling base (14). Counter wound inductors from adjoining coils (1, 2, 3, 4) in the decoupling circuit (7) are interlaced to achieve mutual decoupling between adjoining coils. Each separate coil (1, 2, 3, 4) includes a pair of spaced parallel main conductors (12) located on opposite sides of a cylindrical space (5) enclosed by the coils (1, 2, 3, 4). The decoupling base (14) comprises two meandering conductor bases (8, 9) which are interlaced. Orthogonal main conductors (12) of the coil (1, 2, 3, 4) share a common conductor base (8, 9). The multiple crossings of the paths of the conductor bases (8, 9) reduces mutual coupling effects.
    • 磁共振成像(MRI)相控阵列头线圈(10)包括线圈(1,2,3,4)阵列,去耦电路(7)和去耦基座(14)。 在去耦电路(7)中来自相邻线圈(1,2,3,4)的反绕绕电感器交织以实现相邻线圈之间的相互去耦。 每个分离的线圈(1,2,3,4)包括位于由线圈(1,2,3,4)包围的圆柱形空间(5)的相对侧上的一对隔开的平行主导体(12)。 去耦基座(14)包括两个交织的曲折导体基座(8,9)。 线圈(1,2,3,4)的正交主导体(12)共用公共导体基座(8,9)。 导体基座(8,9)的路径的多个交叉点减少了相互耦合效应。