Mechanism for attaching ultrasonic head of ultrasonic microscope
    2.
    发明授权
    Mechanism for attaching ultrasonic head of ultrasonic microscope 失效
    超声波显微镜超声波头附件机构

    公开(公告)号:US4587848A

    公开(公告)日:1986-05-13

    申请号:US664429

    申请日:1984-10-24

    CPC分类号: G10K11/352 G10K11/30

    摘要: A mechanism for attaching an ultrasonic head of an ultrasonic microscope to a vibration shaft of a vibrator is disclosed. A first connector half to which an R.F. cable is connected is fixedly arranged to the vibration shaft and a second connector half having the ultrasonic head coupled therewith is detachably attached to the first connector half, so that an exchange of the ultrasonic head can be performed in an easy and swift manner without affecting the position and characteristics of the R.F. cable.

    摘要翻译: 公开了一种用于将超声波显微镜的超声波头连接到振动器的振动轴的机构。 一个第一个连接器,一个R.F. 电缆连接固定地设置在振动轴上,并且具有与其耦合的超声波头的第二连接器半部可拆卸地附接到第一连接器半部,使得可以以简单而迅速的方式进行超声波头的交换而不影响 RF的位置和特性 电缆。

    Acoustic lens for use in acoustic microscope
    5.
    发明授权
    Acoustic lens for use in acoustic microscope 失效
    用于声学显微镜的声镜

    公开(公告)号:US4881618A

    公开(公告)日:1989-11-21

    申请号:US56685

    申请日:1987-06-02

    IPC分类号: G10K11/30

    CPC分类号: G10K11/30

    摘要: An acoustic lens for use in an acoustic microscope including a solid state medium for propagating an acoustic wave having a wavelength .lambda. and having opposed end surfaces, an electric-acoustic transducer applied on one end surface of the solid state medium and having a radius a, and a spherical lens portion formed in the other end surface of the solid state medium and having an aperture of a radius w. The length l and the aperture radius w are normalized by the transducer radius a such that Z=l.lambda./a.sup.2 and W=w/a. Values of Z and W are selected from such a region in a first quadrant of the Z-W coordinate system that desired power and/or phase are obtained. The region neighboring the point Z=1 and W=1 is excluded.

    摘要翻译: 一种用于声学显微镜的声透镜,包括用于传播具有波长λ并具有相对端面的声波的固态介质,施加在固态介质的一个端面上并具有半径a的电声换能器, 以及形成在固态介质的另一端面中并具有半径为w的孔径的球面透镜部分。 长度l和孔径半径w通过换能器半径a归一化,使得Z =1λ/ a2和W = w / a。 Z和W的值从Z-W坐标系的第一象限的区域中选择,其中获得期望的功率和/或相位。 排除与Z = 1和W = 1相邻的区域。