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    • 22. 发明申请
    • Methods of screening light chain of antibody
    • 筛选抗体轻链的方法
    • US20060159673A1
    • 2006-07-20
    • US10542839
    • 2004-01-21
    • Tetsuo Kojima
    • Tetsuo Kojima
    • C40B40/10A61K39/395C12N15/74C12N1/21
    • C07K16/005C07K2317/31C07K2317/55
    • The present invention relates to methods of screening for commonly shared light chains, in which the method comprises the steps of (a) generating a host secreting the heavy chain of an antibody that binds to a desired antigen; (b) introducing an antibody light chain library into the host of step (a) to generate libraries presenting antibodies composed of the heavy chain and the light chains; (c) selecting a library presenting antibodies that bind specifically to the desired antigen of step (a); (d) introducing the library selected in step (c) into a host secreting the heavy chain of an antibody that binds to a desired antigen different from the antigen of step (a) to generate libraries that display antibodies composed of the heavy chains and light chains; and (e) selecting a library that displays antibodies that bind specifically to the desired antigen of step (d).
    • 本发明涉及筛选普遍共享的轻链的方法,其中该方法包括以下步骤:(a)产生分泌结合所需抗原的抗体重链的宿主; (b)将抗体轻链文库导入步骤(a)的宿主,以产生呈现由重链和轻链组成的抗体的文库; (c)选择呈递与步骤(a)的所需抗原特异性结合的抗体的文库; (d)将步骤(c)中选择的文库导入分泌与不同于步骤(a)的抗原的期望抗原结合的抗体的重链的宿主,以产生显示由重链和光组成的抗体的文库 链条 和(e)选择显示与步骤(d)的所需抗原特异性结合的抗体的文库。
    • 28. 发明授权
    • Diode laser pumped solid state laser amplifier and diode laser pumped solid state laser
    • 二极管激光泵浦固态激光放大器和二极管激光泵浦固态激光器
    • US07796670B1
    • 2010-09-14
    • US08938700
    • 1997-09-26
    • Shuichi FujikawaTetsuo Kojima
    • Shuichi FujikawaTetsuo Kojima
    • H01S3/09H01S3/091
    • H01S3/0941H01S3/025H01S3/0407H01S3/042H01S3/0602H01S3/061H01S3/08072H01S3/094057H01S3/094084H01S3/2308
    • A diode laser pumped solid-state laser amplifier capable of homogenizing the distribution of heat dissipation levels on a section of a solid-state laser rod and not causing a bifocal phenomenon, and a diode laser pumped solid-state laser using the diode laser pumped solid-state laser amplifier. A diode laser pumped solid-state laser amplifier includes a solid-state laser rod having an optical axis along which a laser beam propagates and includes an active medium therein and a plurality of pumping sources having optical axes that run on a plane orthogonal to the axial core of the solid-state laser rod and are separated by a given distance from the axial core of the solid-state laser rod. When pumping light rays are projected on a plane orthogonal to the axial core of the solid-state laser rod, the plurality of pumping sources are located at equiangular intervals with respect to the axial core of the solid-state laser rod.
    • 一种二极管激光泵浦固态激光放大器,其能够使固态激光棒的一部分上的散热水平分布均匀化并且不引起双焦现象,并且使用二极管激光泵浦固体的二极管激光泵浦固态激光器 状态激光放大器。 二极管激光泵浦固体激光放大器包括固态激光棒,其具有光轴,激光束沿着该光轴传播并且包括其中的有源介质,以及多个泵浦源,其具有在与轴向正交的平面上延伸的光轴 并且与固态激光棒的轴芯分开给定的距离。 当泵浦光线投射在与固态激光棒的轴向芯正交的平面上时,多个泵浦源相对于固态激光棒的轴向芯等角间隔设置。
    • 29. 发明申请
    • SOLID STATE LASER AND WAVELENGTH CONVERSION LASER
    • 固态激光和波长转换激光
    • US20100074296A1
    • 2010-03-25
    • US12513176
    • 2007-12-06
    • Kuniaki IwashiroHiroyuki SuzukiTetsuo KojimaTomotaka Katsura
    • Kuniaki IwashiroHiroyuki SuzukiTetsuo KojimaTomotaka Katsura
    • H01S3/08
    • H01S3/08045G02F1/353G02F1/37G02F2001/3503G02F2001/3507G02F2001/354H01S3/08H01S3/08072
    • Two convex lenses (61, 62), each of which has a focal length “f”, and a 90 degree polarization rotator (5) are interposed between solid-state laser elements (21, 22) of a symmetrical resonator having the two solid-state laser elements (21, 22); a space between the two lenses (61, 62) is made shorter than 2f; and distances between the respective lenses (61, 62) and centers of their adjacent solid-state laser elements (21, 22) are set substantially to “f”, to thus achieve a solid-state laser capable of stably performing high power transverse single mode oscillation desirably having power of 100 W or more. There is acquired a wavelength conversion laser that is further provided with a Q switch (3) and a polarization element (4) and that causes an output fundamental wave laser beam to enter nonlinear elements (91, 92) so as to undergo wavelength conversion, thereby producing a high power harmonic laser beam having a high frequency of; desirably, about 100 kHz.
    • 在具有两个固体的对称共振器的固体激光元件(21,22)之间插入两个具有焦距“f”的凸透镜(61,62)和90度偏振旋转器(5) 状态激光元件(21,22); 使两个透镜(61,62)之间的空间短于2f; 并且各透镜(61,62)与其相邻的固体激光元件(21,22)的中心之间的距离设定为大致为“f”,从而实现能够稳定地执行大功率横向单 期望具有100W或更大的功率的模式振荡。 获得进一步设置有Q开关(3)和偏振元件(4)的波长转换激光器,并且使得输出基波激光束进入非线性元件(91,92)以进行波长转换, 从而产生具有高频率的高功率谐波激光束; 理想地,约100kHz。
    • 30. 发明申请
    • Laser System
    • 激光系统
    • US20070263677A1
    • 2007-11-15
    • US11632164
    • 2005-04-08
    • Eiichi TanakaTetsuo Kojima
    • Eiichi TanakaTetsuo Kojima
    • H01S3/127
    • H01S3/2316H01S3/0057H01S3/0085H01S3/117H01S3/127H01S2301/02
    • In the case where, e.g., because of provision of a high-gain and high-energy Q-switched laser oscillator in a laser system in a MOPA configuration, the duration τz from the time point when oscillation-stage Q switches (13a and 13b) start the gate ON to the time point when a pulse laser beam (18) starts to grow is shorter than the fall time τf of amplification-stage Q switches (13c, 13d, and 13e), by implementing control in such a way that the gate-ON timing of the oscillation-stage Q switches (13a and 13b) lag behind the gate-ON timing of the amplification-stage Q switches (13c, 13d, and 13e) by a predetermined time, the loss in the pulse laser beam (18) at the amplification-stage Q switches (13c, 13d, and 13e) can be prevented, while the gain deterioration due to a spontaneously amplified ray (17) produced in the amplification stage is being suppressed. Therefore, a high-energy pulse laser beam can efficiently be obtained.
    • 在例如由于在MOPA配置中在激光系统中提供高增益和高能量Q开关激光振荡器的情况下,从振荡级Q切换的时间点(13 a和 13 b)通过实施控制,启动栅极ON到脉冲激光束(18)开始增长的时间点比放大级Q开关(13c,13d和13e)的下降时间τf短 使得振荡级Q开关(13a和13b)的栅极导通定时滞后于放大级Q开关(13c,13d和13e)的栅极导通定时,由 在预定时间内,可以防止在放大级Q开关(13c,13d和13e)处的脉冲激光束(18)中的损失,同时由于自发放大的光线(17)产生的增益劣化 在放大阶段被抑制。 因此,可以有效地获得高能脉冲激光束。