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Semrock Master Catalog 2018

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Near Infrared Bandpass Filters<br />

Transmission (%)<br />

100<br />

90<br />

80<br />

70<br />

60<br />

50<br />

40<br />

30<br />

20<br />

10<br />

Center<br />

Wavelength<br />

1535 1550 1570<br />

0<br />

1500 1510 1520 1530 1540 1550 1560 1570 1580 1590 1600<br />

Wavelength (nm)<br />

Transmission &<br />

Bandwidth<br />

Design<br />

Spectra<br />

1535 nm > 90% over 3 nm 6.8 nm<br />

1550 nm > 90% over 3 nm 8.8 nm<br />

1570 nm > 90% over 3 nm 8.9 nm<br />

Nominal<br />

Full-width,<br />

Half-Maximum<br />

LDT specification = 1 J/cm² @1570 nm (10 ns pulse width)<br />

Measuring Light with Wavelengths and Wavenumbers<br />

The “color” of light is generally identified by the distribution<br />

of power or intensity as a function of wavelength λ.<br />

For example, visible light has a wavelength that ranges from<br />

about 400 nm to just over 700 nm. However, sometimes<br />

it is convenient to describe light in terms of units called<br />

“wavenumbers,” where the wavenumber w is typically<br />

measured in units of cm -1 (“inverse centimeters”) and is<br />

simply equal to the inverse of the wavelength:<br />

In applications like Raman spectroscopy, often both wavelength<br />

and wavenumber units are used together, leading to<br />

potential confusion. For example, laser lines are generally<br />

identified by wavelength, but the separation of a particular<br />

Raman line from the laser line is generally given by a<br />

“wavenumber shift” ∆w, since this quantity is fixed by the<br />

molecular properties of the material and independent of<br />

which laser wavelength is used to excite the line.<br />

200 300 400 500 600<br />

<strong>Semrock</strong>’s industry-leading ion-beam-sputtering manufacturing is now available for<br />

making optical filters with precise spectral features (sharp edges, passbands, etc.) at<br />

near-IR wavelengths, with features out to ~ 1700 nm, and high transmission to wavelengths<br />

> 2000 nm. The bandpass filters on this page are ideal as laser source clean-up filters<br />

and as detection filters which pass particular laser wavelengths and virtually eliminate<br />

background over the full InGaAs detector range (850 – 1750 nm). They are optimized for<br />

the most popular “retina-safe” lasers in the 1.5 μm wavelength range, where maximum<br />

permissible eye exposures are much higher than in the visible or at the 1.06 μm neodymium<br />

line. Applications include laser radar, remote sensing, rangefinding, and laser-induced<br />

breakdown spectroscopy (LIBS).<br />

Near-IR bandpass filters are a good match for Er-doped fiber and Er-doped glass lasers at 1535 nm, r-doped fiber and InGaAsP semiconductor lasers at<br />

1550 nm, and Nd:YAG-pumped optical parametric oscillators (OPO’s) at 1570 nm.<br />

OD 5<br />

Blocking Range<br />

850 – 1519 nm<br />

1550 – 1750 nm<br />

850 – 1534 nm<br />

1565 – 1750 nm<br />

850 – 1554 nm<br />

1585 – 1750 nm<br />

When speaking of a “shift” from a first known wavelength λ 1<br />

to a second known wavelength λ 2<br />

, the resulting wavelength<br />

shift ∆λ is given by<br />

whereas the resulting wavenumber shift ∆w is given by<br />

When speaking of a known wavenumber shift ∆w from a<br />

first known wavelength λ 1<br />

, the resulting second wavelength<br />

λ 2<br />

is given by<br />

Note that when the final wavelength λ 2<br />

is longer than the<br />

initial wavelength λ 1<br />

, which corresponds to a “red shift,” in<br />

the above equations ∆w < 0, consistent with a shift toward<br />

smaller values of w. However, when the final wavelength λ 2<br />

is shorter than the initial wavelength λ 1<br />

, which corresponds<br />

to a “blue shift,” ∆w > 0, consistent with a shift toward<br />

larger values of w.<br />

Wavenumbers (cm -1 )<br />

50,000 33,333 25,000 20,000 16,667 14,286 12,500 11,111 10,000 9,091 8,333<br />

700<br />

Wavelength (nm)<br />

OD 6<br />

Blocking Range Part Number Price<br />

1412 – 1512 nm<br />

1558 – 1688 nm<br />

1426 – 1526 nm<br />

1573 – 1705 nm<br />

1444 – 1546 nm<br />

1593 – 1727 nm<br />

NIR01-1535/3-25 $610<br />

NIR01-1550/3-25 $610<br />

NIR01-1570/3-25 $610<br />

Except for the transmission, bandwidth, and blocking specifications listed above, all other specifications are identical to MaxLine ® specifications on page 99.<br />

TECHNICAL NOTE<br />

800 900 1000 1100 1200<br />

NIR Filters Mirrors Polarizers<br />

Edge<br />

Filters<br />

Dichroic<br />

Beamsplitters<br />

Laser-line<br />

Filters<br />

Laser Diode<br />

Filters<br />

Notch<br />

Filters<br />

Lamp Clean-up<br />

Filters<br />

UV<br />

Near-UV<br />

Visible<br />

Near-IR<br />

101<br />

More

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