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Semrock Master Catalog 2018

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Multiphoton Filters Common Specifications<br />

Common Specifications<br />

Property Emitter LWP Dichroic Comment<br />

Passband<br />

Transmission<br />

Guaranteed > 90% > 93% Averaged over any 50 nm (emitter) or 10 nm<br />

Typical > 95% > 95%<br />

(dichroic) window within the passband. For SWP<br />

dichroic specifications, see page 44 .<br />

Dichroic Reflection LWP N/A > 98% Averaged over any 30 nm window within the reflection<br />

band. For SWP dichroic specifications, see page 44.<br />

Autofluorescence Ultra-low Ultra-low Fused silica substrate<br />

Blocking<br />

Pulse Dispersion<br />

Emitter Orientation<br />

Dichroic Orientation<br />

Emitter filters have exceptional blocking over the Ti:Sapphire laser range as needed to achieve superb<br />

signal-to-noise ratios even when using an extended-response PMT or a CCD camera or other siliconbased<br />

detector.<br />

LWP dichroic beamsplitters are suitable for use with 100 femtosecond Gaussian laser pulses. For SWP<br />

dichroic beamsplitters, see Group Delay Dispersion and Polarization Technical Note at<br />

www.semrock.com<br />

The emitter orientation does not affect its performance; therefore there is no arrow on the ring to<br />

denote a preferred orientation.<br />

For the LWP dichroic, the reflective coating side should face toward detector and sample. For the SWP<br />

dichroic, the reflective coating side should face towards laser as shown in the diagram on page 27.<br />

Fluorophores<br />

Single-band<br />

Sets<br />

Multiband<br />

Sets<br />

Microscope Compatibility<br />

These filters fit most standard-sized microscope cubes from Nikon, Olympus, and Zeiss and may<br />

also be mounted in optical bench mounts. Contact <strong>Semrock</strong> for special filter sizes.<br />

Cubes<br />

TECHNICAL NOTE<br />

Multiphoton Filters<br />

In multiphoton fluorescence microscopy, fluorescent molecules that<br />

tag targets of interest are excited and subsequently emit fluorescent<br />

photons that are collected to form an image. However, in a two-photon<br />

microscope, the molecule is not excited with a single photon as it is in<br />

traditional fluorescence microscopy, but instead, two photons, each<br />

with twice the wavelength, are absorbed simultaneously to excite<br />

the molecule.<br />

Ti:Sapphire<br />

Laser<br />

Source<br />

Laser Beam<br />

Scan Head<br />

Dichroic Beamsplitter<br />

Emitter Filter<br />

Figure 1: Typical<br />

configuration of<br />

a multiphoton<br />

fluorescence<br />

microscope<br />

Laser<br />

Sets<br />

NLO<br />

Filters<br />

As shown in Figure 1, a typical system is comprised of an excitation<br />

laser, scanning and imaging optics, a sensitive detector (usually a<br />

photomultiplier tube), and optical filters for separating the fluorescence<br />

from the laser (dichroic beamsplitter) and blocking the laser light from<br />

the detector (emission filter).<br />

The advantages offered by multiphoton imaging systems include: true<br />

three-dimensional imaging like confocal microscopy; the ability to image<br />

deep inside of live tissue; elimination of out-of-plane fluorescence; and<br />

reduction of photobleaching away from the focal plane to increase<br />

sample longevity. Now <strong>Semrock</strong> has brought enhanced performance<br />

to multiphoton users by introducing optical filters with ultra-high<br />

transmission in the passbands, steep transitions, and guaranteed deep<br />

blocking everywhere it is needed. Given how much investment is<br />

typically required for the excitation laser and other complex elements<br />

of multiphoton imaging systems, these filters represent a simple and<br />

inexpensive upgrade to substantially boost system performance.<br />

Depth 100 µm<br />

Sample<br />

Detector<br />

x-z projection x-y images y-z projection<br />

1<br />

2<br />

Individual<br />

Filters<br />

Dichroic<br />

Beamsplitters<br />

Exciting research using <strong>Semrock</strong> multiphoton filters demonstrates the power of<br />

fluorescent Ca 2+ indicator proteins (FCIPs) for studying Ca 2+ dynamics in live cells using<br />

two-photon microscopy. Three-dimensional reconstructions of a layer 2/3 neuron<br />

expressing a fluorescent protein CerTN-L15. Middle: 3 selected images (each taken<br />

at depth marked by respective number on the left and right).<br />

Image courtesy of Prof. Dr. Olga Garaschuk of the Institute of Neuroscience at<br />

the Technical University of Munich. (Modified from Heim et al., Nat. Methods,<br />

4(2): 127-9, Feb. 2007).<br />

1<br />

2<br />

3<br />

Depth 260 µm<br />

3<br />

1<br />

2<br />

3<br />

Tunable<br />

Filters<br />

47<br />

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