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    OLYMPUS奥林巴斯 BX53-P 偏光显微镜

    OLYMPUS奥林巴斯 BX53-P 偏光显微镜

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    OLYMPUS奥林巴斯 BX53-P 偏光显微镜



    偏振光观察的新标准

    奥林巴斯 BX53-P 偏光显微镜采用 UIS2 无限远校正光学系统和独特的光学设计,在偏光应用中具有出色的性能。扩展的兼容补偿器系列使 BX53-P 显微镜用途广泛,几乎可以处理任何领域的观察和测量应用。

    UIS2 Optics Provide Outstanding Expandability

    Maximizing the advantages of infinity correction, the UIS2 optical system helps prevent the deterioration of optical microscope performance and eliminates magnification factors, even when polarizing elements, like analyzers, tint plates, or compensators, are introduced into the light path. The BX53-P microscope also accepts intermediate attachments available for BX3 series microscopes, as well as cameras and imaging systems.

    UIS2 Optics Provide Outstanding Expandability

    Zonal structure of Plagioclase in quartz diorite. *Scales Indicate actual size of samples

    UIS2 Optics Provide Outstanding Expandability

    Optical texture of MBBA  *Scales Indicate actual size of samples

    Bertrand Lens for Conoscopic and Orthoscopic Observations

    Bertrand Lens for Conoscopic and Orthoscopic Observations

    With a conoscopic observation attachment, switching between orthoscopic and conoscopic observation is simple. It is focusable for viewing of clear back focal plane interference patterns. The Bertrand lens is focusable for clear viewing back focal plane interference patterns. The  field stop makes it possible to consistently obtain sharp conoscopic images.

    An Extensive Range of Compensators and Wave Plates

    Six different compensators are available for measurements of birefringence in rock and mineral thin sections. Measurement retardation level ranges from 0 to 20λ. For easier measurement and high image contrast, Berek and Senarmont
    compensators can be used, which change the retardation level in the entire field of view.

    An Extensive Range of Compensators and Wave Plates

    MEASURING RANGE OF COMPENSATORS
    CompensatorMeasurement RangeApplications
    Thick Berek
    (U-CTB)
    0–11000 nm
    (20λ)
    Measurement of high retardation level (R*>3λ), (crystals, macromolecules,fi ber, etc.)
    Berek
    (U-CBE)
    0–1640 nm
    (3λ)
    Measurement of retardation level (crystals,macromolecules, living organisms, etc.)
    Senarmont
    Compensator
    (U-CSE)
    0–546 nm
    (1λ)
    Measurement of retardation level (crystals, living organisms, etc.);
    enhancement of image contrast (living organisms,etc.)
    Brace-Koehler
    Compensator1/10λ
    (U-CBR1)
    0–55 nm
    (1/10λ)
    Measurement of low retardation level (living organisms, etc.)
    Brace-Koehler
    Compensator1/30λ
    (U-CBE2)
    0–20 nm
    (1/30λ)
    Measurement of image contrast (living organisms,etc.)
    Quartz Wedge
    (U-CWE2)
    500–2200 nm
    (4λ)
    Approximate measurement of retardation level (crystal, macromolecules, etc.)
    *R = retardation level
    For more accurate measurement, we recommend that compensators (except U-CWE2) be used together with the interference fi lter 45-IF546

    Minimal Strain Optics

    Minimal Strain Optics

    Our polarized light objectives reduce internal strain to a minimum. This means a higher EF value, resulting in excellent image contrast.

    Robust and Accurate Rotating Stage

    The rotating-centering mechanism attached to the rotary stage  enables smooth rotation of a specimen. In addition, there is a click-stop mechanism at each 45 degrees for precise measurement. With the optional dual-mechanical stage, discreet X-Y movement is possible.

    Dual-mechanical Stage

    Dual-mechanical Stage

    观察方法明场

    偏光

    简易偏光
    聚焦聚焦机制载物台聚焦
    载物台机械式精密可旋转式载物台
    • 旋转角度:360度
    聚光镜手动偏光聚光镜NA 0.9 / WD 1.3毫米(载玻片1.5毫米)(4X-100X)
    观察筒宽视场(FN 22)三目观察筒


    倾斜式三目观察筒
    尺寸(宽×深×高)

    274 (W) x 436 (D) x 535 (H) mm
    重量

    16 kg




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