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Semrock Master Catalog 2018

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Fluorophores<br />

Single-band<br />

Sets<br />

Multiband<br />

Sets<br />

Cubes Laser<br />

Sets<br />

VersaChrome ® Tunable Filters<br />

TECHNICAL NOTE<br />

Tunable Bandpass Filters<br />

Thin-film filters are the ideal solution for wavelength selection in most optical systems due to exceptionally high transmission<br />

at passband wavelengths (close to 100%), very steep spectral edges, and blocking of optical density 6 or higher over wide<br />

spectral regions for maximum noise suppression. However, thin-film filters are considered to be “fixed” filters only, such<br />

that changing the spectral characteristics requires swapping filters, thus constraining system size, speed, and flexibility for<br />

systems that require dynamic filtering. Diffraction gratings are often used when wavelength tuning is required, but gratings<br />

exhibit inadequate spectral discrimination, have limited transmission, are polarization dependent, and are not capable of<br />

transmitting a beam carrying a two-dimensional image since one spatial dimension carries spectral information.<br />

Fluorescence microscopy and other fluorescence imaging and quantitation applications, hyperspectral imaging, highthroughput<br />

spectroscopy, and fiber-optic telecommunications systems can all benefit from tunable optical filters with the<br />

spectral and two-dimensional imaging performance characteristics of thin-film filters and the center wavelength tuning<br />

flexibility of a diffraction grating. T There exist several technologies that combine some of these characteristics, including<br />

liquid-crystal tunable filters, acousto-optic tunable filters, and linear-variable filters, but none are ideal and all have significant<br />

additional limitations.<br />

<strong>Semrock</strong> has developed a revolutionary patented optical filter technology: thin-film optical filters that are tunable over a<br />

very wide range of wavelengths by adjusting the angle of<br />

λ<br />

incidence with essentially no change in spectral performance.<br />

As the diagrams (below) indicate, both edge filters and bandpass filters with wide tunability are possible.<br />

T<br />

60° 0° 60° 0°<br />

λ<br />

T<br />

λ<br />

NLO<br />

Filters<br />

Individual<br />

Filters<br />

Dichroic<br />

Beamsplitters<br />

Tunable<br />

Filters<br />

It is well-known that the spectrum of any thin-film filter shifts toward shorter wavelengths when T the angle of incidence<br />

of light upon the filter is increased from 0° (normal incidence) to larger angles. In general, however, the filter spectrum<br />

becomes highly distorted at larger angles, and the shift can be significantly different for s- and p-polarized light, also leading<br />

to a strong polarization dependence at higher angles. The graph on the left shows the spectrum of a typical fluorescence<br />

filter at six different angles of incidence ranging from 0° to 60°. Note that for angles greater than about 30° transmission for<br />

s-polarized light is approximately 0% and the ripple for p-polarized light is intolerably high.<br />

λ<br />

Typical<br />

VersaChrome<br />

In contrast, the spectrum of a<br />

60° 50° 40° 30° 20° 0°<br />

<strong>Semrock</strong> VersaChrome bandpass<br />

100<br />

60° 50° 40° 30° 20° 0°<br />

100<br />

filter (right) maintains high<br />

90<br />

90<br />

transmission, steep edges, and<br />

80<br />

80<br />

excellent out-of-band blocking over<br />

70<br />

70<br />

the full range of angles from 0 to<br />

60<br />

60<br />

60°. At the heart of this invention<br />

50<br />

50<br />

is <strong>Semrock</strong>’s discovery of a way<br />

40<br />

40<br />

to make very steep edge filters<br />

30<br />

30<br />

(both long-wave-pass, or “cut-on,”<br />

20<br />

20<br />

and short-wave-pass, or “cut-off,”<br />

10<br />

10<br />

type filters) at very high angles<br />

0<br />

450 470 490 510 530 550 570 590 0<br />

of incidence with essentially no<br />

450 470 490 510 530 550 570 590<br />

Wavelength (nm)<br />

polarization splitting and nearly<br />

Wavelength (nm)<br />

equal edge steepnesses for both<br />

polarizations of light. An equally<br />

significant and related property is that the high edge steepness values for both polarizations and the lack of polarization<br />

splitting apply at all angles of incidence from normal incidence (0°) to very high angles. As a consequence, it is possible<br />

to angle tune the edge filter, or a combination of edge filters, over this full range of angles with little to no change in the<br />

properties of the edges regardless of the state of polarization of the light passing through the filter. And thus it is now<br />

possible to make tunable thin-film filters which operate over a very wide range of wavelengths – <strong>Semrock</strong>’s VersaChrome<br />

series of filters are specified with a tuning range of at least 11% of the filter edge or center wavelength at normal incidence.<br />

Transmission (%)<br />

Transmission (%)<br />

More<br />

78

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