Semrock Master Catalog 2018

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RazorEdge ® Short Wave Pass Raman Edge Filters Polarizers Mirrors NIR Filters Edge Filters Dichroic Beamsplitters Laser-line Filters Laser Diode Filters Notch Filters Lamp Clean-up Filters 25 mm and 50 mm Diameters Laser Line Transition Width Passband Part Number Price 532.0 nm < 186 cm –1 350.0 – 525.2 nm SP01-532RU-25 $795 561.4 nm < 176 cm –1 400.0 – 554.1 nm SP01-561RU-25 $695 632.8 nm < 160 cm –1 372.0 – 624.6 nm SP01-633RU-25 $795 785.0 nm < 129 cm –1 400.0 – 774.8 nm SP01-785RU-25 $695 50 mm SWP Edge Filters - $695 Wavelengths above 50 mm SWP Edge Filters - $795 Wavelengths above These unique filters are ideal for Anti-Stokes Raman applications. An addition to the popular high-performance RazorEdge family of steep edge filters, these short-wave-pass filters are designed to attenuate a designated laser-line by six orders of magnitude, and yet maintain a typical edge steepness of only 0.5% of the laser wavelength. Both short and long-wave-pass RazorEdge filters are perfectly matched to Semrock’s popular MaxLine ® laser-line cleanup filters. U.S. Patent No. 7,068,430 SP01-___RU-50 SP01-___RU-50 See spectra graphs and ASCII data for all of our filters at www.semrock.com PRODUCT NOTE RazorEdge and MaxLine ® are a Perfect Match The MaxLine (see page 98) and RazorEdge U-grade (see page 92) filters make an ideal filter pair for applications like Raman spectroscopy – they fit together like hand-in-glove. The MaxLine filter spectrally “cleans up” the excitation laser light before it reaches the sample under test – allowing only the desired laser line to reach the sample – and then the RazorEdge filter removes the laser line from the light scattered off the sample, while efficiently transmitting desired light at wavelengths very close to the laser line. Typical measured spectral curves of 785 nm filters on a linear transmission plot demonstrate how the incredibly steep edges and high transmission exhibited by both of these filters allow them to be spectrally positioned very close together, while still maintaining complementary transmission and blocking characteristics. The optical density plot (for explanation of OD, see page 107) illustrates the complementary nature of these filters on a logarithmic scale using the theoretical design spectral curves. The MaxLine filter provides very high transmission (> 90%) of light immediately in the vicinity of the laser line, and then rapidly rolls off to achieve very high blocking (> OD 5) at wavelengths within 1% of the laser line. The RazorEdge filter provides extremely high blocking (> OD 6) of the laser line itself, and then rapidly climbs to achieve very high transmission (> 90%) of the desired signal light at wavelengths only 1% away from the laser line. If you are currently using an E-grade RazorEdge filter and need a laser clean-up filter, please contact Semrock. $1985 $2255 ACTUAL MEASURED DATA FROM A 632.8 nm RAZOREDGE FILTER Transmission Transmission (%) (%) Optical Optical Density Density 100 Transmission (%) 100 90 80 70 60 50 40 30 20 10 Measured Laser Line 0 400 450 500 550 600 650 700 750 Wavelength (nm) 90 100 Typical 80 90 Measured Data 70 Typical 80 Measured Data 60 70 50 60 40 50 30 40 785 MaxLine 20 30 785 RazorEdge 10 785 MaxLine 20 785 RazorEdge 0 10700 720 740 760 780 800 820 840 860 880 900 0 Wavelength (nm) 700 720 740 760 780 800 820 840 860 880 900 0 01 12 23 34 45 56 67 78 8 Wavelength (nm) 1% 1% Laser Line 785 MaxLine 785 RazorEdge Laser Line 785 MaxLine 777 781 785 789 793 785 797RazorEdge 801 805 Wavelength (nm) Guaranteed high transmission for Guaranteed RazorEdge and high transmission high blocking for for RazorEdge MaxLine filter and high blocking for MaxLine filter 777 781 785 789 793 797 801 805 Wavelength (nm) More 94
RazorEdge ® Common Specifications RazorEdge Specifications Properties apply to all long-wave-pass and short-wave-pass edge filters unless otherwise noted Property Specification Comment Edge Steepness (typical) E-grade 0.2% of laser wavelength U-grade 0.5% of laser wavelength Blocking at Laser Wavelength > 6 OD OD = - log 10 (transmission) Transition Width E-grade < 0.5% of laser wavelength U-grade < 1% of laser wavelength Measured from OD 6 to 50%; Up to 0.8% for 248-300 nm filters and 3.3% for 224 nm filter Measured from laser wavelength to 50% transmission wavelength; < 4.5% for 224 nm filter Guaranteed Passband Transmission > 93% Except > 90% for 224 – 325 nm filters; Averaged over the Passband Typical Passband Transmission > 98% Angle of Incidence 0.0° ± 2.0° Range for above optical specifications Cone Half Angle < 5° Rays uniformly distributed about 0° Angle Tuning Range [1] -0.3% of Laser Wavelength (-1.6 nm or + 60 cm -1 for 532 nm) Wavelength “blue shift” attained by increasing angle from 0° to 8° Laser Damage Threshold 0.5 J/cm 2 @ 266 nm 10 ns pulse width 1 J/cm 2 @ 532 nm Tested for 266 and 532 nm filters only (see page 108) Clear Aperture >22 mm (or > 45 mm) 25.0 + 0.0 / -0.1 mm Outer Diameter (or 50.0 + 0.0 / -0.1 nm) Black-anodized aluminum ring Substrate Thickness 2.0 mm Overall Thickness 3.5 ± 0.1 mm Black-anodized aluminum ring (thickness measured unmounted) Beam Deviation < 10 arcseconds [1] For small angles (in degrees), the wavelength shift near the laser wavelength is Dl (nm) = -5.0 x 10 –5 x l L x q 2 and the wavenumber shift is D(wavenumbers) (cm –1 ) = 500 x q 2 / l L , where l L (in nm) is the laser wavelength. See Wavenumbers Technical Note on page 101. General Specifications (all RazorEdge filters) Property Specification Comment Coating Type Reliability and Durability “Hard” ion-beam-sputtered Ion-beam-sputtered, hard-coated technology with epoxy-free, single-substrate construction for unrivaled filter life. RazorEdge filters are rigorously tested and proven to MIL-STD-810F and MIL-C-48497A environmental standards. Transmitted Wavefront Error < λ / 4 RMS at λ = 633 nm Peak-to-valley error < 5 x RMS value measured within clear aperture Surface Quality 60-40 scratch-dig Temperature Dependence < 5 ppm / °C Substrate Material Filter Orientation TECHNICAL NOTE RazorEdge Filter Layouts Ultra-low autofluorescence fused silica Only the unique RazorEdge Dichroic beamsplitter reflects a standard laser line incident at 45° while transmitting longer Raman-shifted wavelengths with an ultrasteep transition far superior to anything else available on the open market. The guaranteed transition width of < 1% of the laser wavelength for U-grade (regardless of polarization) makes these filters a perfect match to our popular normal-incidence RazorEdge ultrasteep long-wave-pass filters. For mounted filters, arrow on ring indicates preferred direction of propagation of transmitted light. For rectangular dichroics, reflective coating side should face toward light source and sample. Standard Raman spectroscopy layout Laser Laser MaxLine Laser MaxLine Transmitting Laser Filter Transmitting Filter Spectrometer Spectrometer Sample Sample RazorEdge Laser RazorEdge Blocking Laser Filter Blocking Filter NIR Filters Mirrors Polarizers Edge Filters Dichroic Beamsplitters Laser-line Filters Laser Diode Filters Notch Filters In order for the two-filter configuration to work, the 45° beamsplitter must be as steep as the laser-blocking filter. Traditionally thinfilm filters could not achieve very steep edges at 45° because of the “polarization splitting” problem – the edge position tends to be different for different polarizations of light. However, through continued innovation in thin-film filter technology, Semrock has been able to achieve ultrasteep 45° beamsplitters with the same steepness of our renowned RazorEdge laser-blocking filters: the transition from the laser line to the passband of the filter is guaranteed to be less than 1% of the laser wavelength (for U-grade filters). Imaging system with high-NA collection optics Laser Laser MaxLine Laser MaxLine Transmitting Laser Filter Transmitting Filter Spectrometer Spectrometer Sample Sample RazorEdge Laser RazorEdge Blocking Laser Filter Blocking Filter RazorEdge RazorEdge Dichroic Beamsplitter Dichroic Beamsplitter High-NA High-NA Optics Optics Lamp Clean-up Filters 95 More
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Semrock 2018 Master Catalog Everyth
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Welcome to the 2018 Master Catalog
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T T T T Laser & Optical System Filt
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SearchLight Optimization Calculator
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The Semrock Advantage Proven Reliab
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BrightLine ® Single-band Sets When
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BrightLine ® Single-band Sets for
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BrightLine ® Multiband Sets for Po
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BrightLine ® Single-band Sets Filt
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TECHNICAL NOTE Ultraviolet (UV) Flu
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BrightLine ® Single-band Sets for
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Qdot ® Single-band Filter Sets Fil
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BrightLine ® FRET Single-band Sets
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BrightLine ® Basic TM Best-value S
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(continued from previous page) Fluo
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BrightLine ® Multiband LED Filter
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BrightLine ® Multiband Fluorescenc
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BrightLine ® Multiband Fluorescenc
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Fluorescence Filter Cubes See onlin
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BrightLine ® Laser Filter and Set
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BrightLine ® Laser Fluorescence Mu
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BrightLine ® Laser Fluorescence Fi
Page 45 and 46: TECHNICAL NOTE Sputtered Thin-film
Page 47 and 48: BrightLine ® Multiphoton LaserMUX
Page 49 and 50: Multiphoton Filters Common Specific
Page 51 and 52: BrightLine ® Single-band Bandpass
Page 59 and 60: BrightLine ® Long / Short pass Sin
Page 61 and 62: BrightLine ® Multiband Bandpass Fi
Page 63 and 64: BrightLine ® Multiband Bandpass Fi
Page 65 and 66: BrightLine ® Single-edge Dichroic
Page 67 and 68: BrightLine ® Multiedge Dichroic Be
Page 69 and 70: BrightLine ® Dichroic Beamsplitter
Page 71 and 72: Single-band Sets Fluorophores (cont
Page 73 and 74: BrightLine ® Super-resolution / TI
Page 75 and 76: BrightLine ® Laser Multiedge Dichr
Page 77 and 78: LaserMUX TM Beam Combining Filters
Page 79 and 80: TECHNICAL NOTE Measurement of Optic
Page 81 and 82: VersaChrome ® Tunable Filters TECH
Page 83 and 84: VersaChrome ® Tunable Bandpass Fil
Page 85 and 86: VersaChrome Edge TM Tunable Filters
Page 87 and 88: Laser Wavelength Reference Table La
Page 89 and 90: Polarization Filters Common Specifi
Page 91 and 92: General Purpose Mirrors Semrock gen
Page 93 and 94: EdgeBasic TM Long / Short Wave Pass
Page 95: Edge Steepness and Transition Width
Page 99 and 100: Filter Types for Raman Spectroscopy
Page 101 and 102: MaxLine ® Laser-line Spectra and S
Page 103 and 104: Near Infrared Bandpass Filters Tran
Page 105 and 106: StopLine ® Single-notch Filter Com
Page 107 and 108: TECHNICAL NOTE Filter Spectra at No
Page 109 and 110: Working with Optical Density Optica
Page 111 and 112: LEARN MORE WITH OUR VIDEO COLLECTIO
Page 113 and 114: The Physics of Pixel Shift Pixel sh
Page 115 and 116: Get the Right Solution, Right Now W
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Semrock Master Catalog 2018

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