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    • 3. 发明公开
    • COMBINED IMAGING SYSTEM AND MRI COMPATIBLE LASER SCANNING MICROSCOPE
    • 组合成像系统和MRI兼容的激光扫描显微镜
    • EP3221707A1
    • 2017-09-27
    • EP15860226.8
    • 2015-11-18
    • Femtonics Kft.
    • RÓZSA, BalázsKATONA, Gergely
    • G01Q60/00G02B21/00G01N24/00
    • G01R33/4808G01R33/381G02B21/002
    • The subject of the invention relates to a combined imaging system (10') that includes a laser scanning microscope (50, 50'), and a measuring device with a lower resolution than the resolution of the laser scanning microscope (50, 50') and that measures over a larger spatial scale than the spatial scale of the laser scanning microscope (50, 50'). The subject of the invention also relates to an MRI compatible laser scanning microscope which comprises: deflecting means (24') for deflecting a laser beam (13), objective (28'), adjustable objective arm (38), distance adapter (39) and at least one detector (30'). The essence of the MRI compatible laser scanning microscope is that at least the objective (28'), the adjustable objective arm (38), the distance adapter (39) and the at least one detector (30') are made from non-magnetisable materials and the deflecting means (24') is magnetically shielded.
    • 本发明的主题涉及包括激光扫描显微镜(50,50')和分辨率低于激光扫描显微镜(50,50')的分辨率的测量装置的组合成像系统(10'), 并且在比激光扫描显微镜(50,50')的空间尺度更大的空间尺度上进行测量。 本发明的主题还涉及MRI兼容的激光扫描显微镜,其包括:用于偏转激光束(13)的偏转装置(24'),物镜(28'),可调物镜臂(38),距离适配器(39) 和至少一个检测器(30')。 MRI兼容激光扫描显微镜的本质在于至少物镜(28'),可调物镜臂(38),距离适配器(39)和至少一个检测器(30')由不可磁化的 材料和偏转装置(24')被磁屏蔽。
    • 7. 发明公开
    • COMPENSATOR SYSTEM AND METHOD FOR COMPENSATING ANGULAR DISPERSION
    • 补偿器系统和方法,用于补偿色散角的
    • EP2798401A1
    • 2014-11-05
    • EP12709692.3
    • 2012-01-05
    • Femtonics Kft.
    • RÓZSA, BalázsKATONA, GergelyVERESS, MátéMAÁK, PálSZALAY, Gergely
    • G02F1/33G02B21/00G02B27/00
    • G02F1/33G02B5/04G02B21/002G02B21/0036G02B27/0031G02B27/30
    • The invention relates to a compensator system adapted to compensate for the angular dispersion of electromagnetic beams deflected by at least one acousto-optic deflector of an optical system, wherein the angular dispersion of each deflected beam is dependent on the deflection angle obtained by the deflecting acoustic frequency of the acousto-optic deflector, characterized in that the compensator system comprises: —a first lens group for spatially separating the deflected beams of different deflection angle and angular dispersion by focusing the beams substantially into the focal plane, —a compensator element having a first surface and a second surface, and being arranged such that the first surface of the compensator element lies substantially in the focal plane of the first lens group, and the first and second surfaces of the compensator element have nominal radiuses R1 and R2 that together work as prisms with tilt angles β and prism opening angles αp that vary with the distance from the optical axis so as to compensate for the angular dispersion of the spatially separated deflected beams, —a second lens group arranged so as to substantially parallelize the different wavelength components of each deflected beam exiting the compensator element while maintaining the angular variation of the beams deflected at different acoustic frequencies. The invention further relates to method for compensating for the angular dispersion of electromagnetic beams deflected by at least one acousto-optic deflector of an optical system, wherein the angular dispersion of each deflected beam is dependent on the deflection angle obtained by the deflecting acoustic frequency, characterized by —spatially separating the deflected beams of different deflection angle and angular dispersion by focusing the beams via a first lens group substantially into the focal plane of the first lens group, —compensating for the angular dispersion of the spatially separated deflected beams in accordance with the angular dispersion of the given beam, —substantially parallelizing the spectral components of each deflected beam while maintaining the angular variation of the beams deflected at different acoustic frequencies.