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    • 3. 发明授权
    • Optical scanning with aberration correction
    • 具有像差校正的光学扫描
    • US06496452B2
    • 2002-12-17
    • US09741920
    • 2000-12-20
    • Sjoerd StallingaJoris Jan VrehenJeroen Wals
    • Sjoerd StallingaJoris Jan VrehenJeroen Wals
    • G11B700
    • G11B7/1369G11B7/0956G11B7/13927
    • An optical head scans the information layer (3) of an optical record carrier (1) by means of a radiation beam (13). Optical aberrations in the beam such as coma and spherical aberration, caused by tilt and thickness variations in the optical disc respectively, are compensated by an aberration compensator (27) arranged in the radiation beam. The tilt or thickness variation is measured by a detector (30) and used to control the aberration compensator. The radiation beam is focused onto the information layer by an objective system (11). A displacement of the objective system in the transverse direction (26) as used for radial tracking of the optical beam, causes a mismatch between the wavefront to be compensated and the wavefront introduced by the aberration compensator (27). The detrimental effects of the mismatch are reduced by compensating only part of the aberration. The degree of compensation depends on the maximum displacement of the objective system and the tolerable wavefront error.
    • 光头通过辐射束(13)扫描光学记录载体(1)的信息层(3)。 由光盘中的倾斜和厚度变化引起的诸如彗差和球面像差的光束中的光学像差由布置在辐射束中的像差补偿器(27)补偿。 倾斜或厚度变化由检测器(30)测量并用于控制像差补偿器。 辐射束通过客观系统(11)聚焦到信息层上。 用于光束的径向跟踪的​​横向(26)的物镜系统的位移导致要补偿的波前与由像差补偿器(27)引入的波阵面之间的失配。 通过仅补偿部分像差来减少不匹配的有害影响。 补偿程度取决于物镜系统的最大位移和允许的波前误差。
    • 6. 发明授权
    • Colour management for biological samples
    • 生物样品的色彩管理
    • US08649581B2
    • 2014-02-11
    • US13124693
    • 2009-10-16
    • Maarten M. J. W. Van HerpenDirk L. J. VossenSjoerd StallingaBernardus H. W. HendriksErik M. H. P. Van Dijk
    • Maarten M. J. W. Van HerpenDirk L. J. VossenSjoerd StallingaBernardus H. W. HendriksErik M. H. P. Van Dijk
    • G06K9/00
    • G06T11/001H04N1/62
    • A method of determining a color transformation for images of biological material includes preparing a first set of biological test objects using a first preparation method, and preparing a second set of biological test objects using a second preparation method. Each test object in the second set of test objects corresponding to a counterpart test object in the first set of test objects, the test object and its counterpart being of the same biological type of material. For each test object in the first and second set of test objects, the color of the test object is determined thereby generating a first and second set of colors The method further includes generating a conversion table indicating a mapping between the colors in the first set of colors and the corresponding colors in the second set of colors. The first and second preparation methods include first and second staining methods, respectively.
    • 确定生物材料的图像的颜色变换的方法包括使用第一制备方法制备第一组生物测试对象,并使用第二制备方法制备第二组生物测试对象。 第二组测试对象中的每个测试对象对应于第一组测试对象中的对应测试对象,测试对象及其对应物具有相同的生物类型的材料。 对于第一和第二组测试对象中的每个测试对象,确定测试对象的颜色,从而生成第一和第二组颜色。该方法还包括生成表示第一组中的颜色之间的颜色之间的映射的转换表 颜色和相应的颜色在第二组颜色。 第一和第二种制备方法分别包括第一和第二染色方法。
    • 9. 发明申请
    • TWO-DIMENSIONAL ARRAY OF RADIATION SPOTS FOR AN OPTICAL SCANNING DEVICE
    • 用于光学扫描装置的两维辐射阵列阵列
    • US20110019064A1
    • 2011-01-27
    • US12933166
    • 2009-03-16
    • Sjoerd Stallinga
    • Sjoerd Stallinga
    • H04N5/225G02B21/06
    • G02B21/004G02B26/10
    • The invention relates to an optical scanning device (10) comprising: a spot generator (20) for generating a two-dimensional array (8) of radiation spots at lattice points Pmn=mT1+nT2 (m=1 to L1, n=1 to L2) where T 1 is a first lattice vector and T2 is a second lattice vector, and scanning means for scanning a sample (26) through the array of radiation spots in a scanning direction such that the radiation spots trace essentially equidistant lines (81, 82, 83) relative to the sample. According to the invention, the angle γ between the scanning direction and the first lattice vector T1 is at most as large as the angle between the scanning direction and the second lattice vector T2, and the ratio L1/L2 is less than 0.6. According to a preferred embodiment, L1 differs from Λ by less then 1.0 or L1 equals Λ with a tolerance of 10% or, Λ being defined by √2 D/R=(1+Λ2) Λ, D being the length of a lattice diagonal and R being the resolution. The invention further relates to an optical scanning method.
    • 本发明涉及一种光学扫描装置(10),包括:点阵发生器(20),用于在格点Pmn = mT1 + nT2(m = 1至L1,n = 1)处产生辐射点的二维阵列(8) 到L2),其中T 1是第一晶格矢量,T2是第二晶格矢量;以及扫描装置,用于通过扫描方向上的辐射点阵列扫描样品(26),使得辐射点基本上等距线(81 ,82,83)。 根据本发明,扫描方向与第一格子矢量T1之间的角度γ与扫描方向和第二格子矢量T2之间的角度最大,并且比率L1 / L2小于0.6。 根据优选实施例,L1与Λ不同于1.0或L1等于Λ,其公差为10%,或Λ由√2D / R =(1 +Λ2)Λ定义,D是格子的长度 对角线和R是分辨率。 本发明还涉及一种光学扫描方法。