Research Inverted System Microscope IX71/IX81 : Features (3)
- Live Cell Fluorescence Imaging
- Optical Port system
- New FL system (1)
- New FL system (2)
- DIC system
- RC/PH System
- Basic Characteristics
- Motorized Units
- Live Cell Imaging System
Improved S/N ratio enables efficient detection of even weak fluorescence.
Better S/N ratio delivers brighter, higher-contrast images in fluorescence observation.
The ideal microscope allows bright, high contrast fluorescence observation from the minimum amount of excitation light in order to minimize cell damage or fluorescence fading. However, to detect a weak fluorescence signal (S) efficiently, all other light noise (N) must be reduced. The higher this S/N ratio, the brighter and clearer the observation image from weak excitation light.
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Fluorescence Observation Units

High S/N ratio objective with reduced autofluorescence
Olympus
offers a range of other high numerical aperture
objectives whose reduced autofluorescence and specially selected
glass contribute to improved fluorescence S/N ratios.
Especially the PLAPON60XO has outstanding N.A., which is 1.42.
| N.A. | W.D. (mm) | |
|---|---|---|
| UPLSAPO 10X2 | 0.40 | 3.1mm |
| UPLSAPO 20X | 0.75 | 0.6mm |
| UPLSAPO 40X2 | 0.95 | 0.18mm |
| UPLSAPO 60XO | 1.35 | 0.15mm |
| UPLSAPO 100XO | 1.40 | 0.13mm |
| PLAPON60 XO | 1.42 | 0.15mm |
| UPLFLN40XO | 1.30 | 0.2mm |
| LUCPLFLN 20X | 0.45 | 6.6 — 7.8mm |
| LUCPLFLN 40X | 0.60 | 2.7 — 4mm |
| LUCPLFLN 60X | 0.70 | 1.5 — 2.2mm |

High-performance fluorescence mirror units for fluorescent proteins
Olympus has developed outstanding filter coating technology,
which gives the high efficient transmission and the reflection as well
as sharp cut off characteristics. This newly developed coating
results in optimized mirror units for the various fluorochromes
included ECFP/EGFP/EYFP/DsRed.

Ring slit illumination unit to reduce noise / IX2-RFRS

The ring slit illumination IX2-RFRS makes the ring shape
illumination on the objective to allow excitation light to pass through
the objectives outer portion
to not to excite the objective
auto-fluorescence generated
at the center of an objectives
* Patent pending.
| Illumination | Normal | Annular |
|---|---|---|
| SIGNAL | 408 | 479 |
| NOISE | 36 | 18 |
| S/N | 11.3 | 26.6 |


Improved performance of interference membrane-type fluorescence mirror unit
The S/N ratio of certain interference type fluorescence mirror
units is now improved, thanks to the application of new coating
technology to narrow the gap between excitation (Ex) and emission
(Em). The line-up has been extended for wide variety of choice.
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Glass reflector captures fluorescence of multiple color dyes

A multi-band dichromatic mirror is normally used to obtain multicolor
images of multiple stained fluorescent samples by using filter
wheels on the excitation and emission sides. However, this kind of
mirror encounters the problem that each fluorescence image gets
darker as the number of color dyes increase, because the
transmission spectrum becomes narrower and the transmittance
falls to lower than 90% at best. Olympus has therefore developed
the world's first glass reflector that is not wavelength-dependent,
offering a high transmittance of 94% across a wide wavelength
range from 430nm to 700nm. Used in combination with the filter
wheels on the excitation and emission sides, a wider variety of color
dyes can be used and
fluorescence images are captured
more efficiently.
*Special order basis product
| Glass reflector specifications |
|---|
| 26X38mm (t=1mm) glass substrate |
| Transmittance 94% (at 430-700nm) 26X38mm |
| * Observations through eyepieces may have some restrictions |

Stray light reducing function equipped on all mirror units

The slight transmission of stray light when excitation light is
reflected in the dichromatic mirror causes a rise in the level of noise.
Olympus mirror units absorb more than 99% of this stray light
through their light absorber.
High performance mirror units
The sharp reactions of the dichromatic mirror in the new mirror
unit minimize crossover with the excitation filter and reduce excitation
light leakage to less than a tenth of our conventional models. Combined
with the light absorbing mechanism (which absorbs more than 99% of stray
light), a high S/N ratio is achieved without the need for any special mechanism
to prevent excitation light leakage.
