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17 protocols using hl 2000 fhsa

1

Optical Characterization of Color Filters

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The completed Al pattern was visually evaluated under a high-resolution field emission scanning electron microscope (FESEM S-4800, Hitachi). The transmission spectra were checked for different polarizations through the launching of a halogen-lamp (HL-2000-FHSA, Ocean Optics) collimated beam, which was properly polarized through a calcite crystal polarizer (GTH 10M-A, Thorlabs), toward the prepared filter that had been mounted on a motorized rotation stage via a focusing lens. The optical output was captured by a spectrometer (Avaspec-3648, Avantes) via a multimode fiber. The images that are related to each pixel of the color filter were captured using a digital microscope (Leica DM6000 M).
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2

Characterization of AgNP-Embedded Microgels

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A Hitachi H-7650 transmission electron microscope (TEM, Japan) with an accelerating voltage of 200 kV was utilized to obtain TEM images. X-Ray Photoelectron Spectroscopy (XPS) was performed on a Kratos AXIS Ultra spectrometer equipped with a monochromated Al Kα ( = 1486.6 eV) X-ray source (Kratos Analytical, Manchester, UK). Nicolet Magna 750 FTIR Spectrometer and Nic-Plan FTIR Microscope (Nicolet, USA) with pure KBr as the background was applied to record Fourier transform infrared (FTIR) spectra (400–4000 cm−1). The microgel samples for TEM, XPS and FTIR characterization were prepared using the procedure described below for generating AgNPs in the etalons with two modifications. First, to obtain sufficient sample for analysis we didn't wash the slide after microgel painting, which yielded a thick microgel layer for AgNP generation. Second, the etalon's top Au layer was not deposited on the microgels, which allowed for their easy removal from the surface while avoiding potential contamination. Reflectance measurements were conducted using a USB2000+ spectrophotometer, an HL-2000-FHSA tungsten light source, and an R400-7-VISNIR optical fiber reflectance probe, all from Ocean Optics (Dunedin, FL). The spectra were recorded using Ocean Optics Spectra Suite spectroscopy software over a wavelength range of 400–1000 nm.
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3

Multimodal Cerebral Monitoring System

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The bespoke hybrid optical system combines bNIRS (developed in UCL, UK) for the monitoring oxCCO along with measures of cerebral oxygenation, and DCS for monitoring cerebral blood flow (BFI, blood flow index), custom-made by Hemophotonics, S.L. (Barcelona, Spain).
The bNIRS consists of a tungsten halogen lamp light source (HL-2000-FHSA, Ocean Optics), a 700-nm long pass filter, and a custom-made micro spectrometer (644–917 nm, cooled CCD, 1024 pixels, Wasatch Photonics). The DCS system consists of a 785 nm long coherence (>8 m) diode laser and a 4-channel photon-counting detector. To guide the light to the piglet, a multimode fibre (400 µm, 0.37 Numerical Aperture (NA)) is used for the DCS laser, and a fibre bundle of 2.5 mm (30 µm fibres, 0.55 NA) is used for the bNIRS halogen source. For the detection, a fibre bundle of four single-mode fibres (3.5 µm, 0.13 NA) is used to direct the light to the four detectors for the DCS, and to the bNIRS (2 mm bundle of 30 µm fibres, 0.55 NA). All the fibres were made by Fibreoptic Systems and were 3 m long. A custom 3D-printed probe holder was designed to attach the fibres on the head of the piglet, with a source-detector separation of 3 and 2 cm for the bNIRS and the DCS, respectively. We use computer-controlled shutters to time multiplex the two instruments, allowing fast sequential measurements from each modality.
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4

Angle-Resolved Optical Characterization

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Transmission
spectra were
recorded with a V-770 (JASCO) spectrophotometer. For angle-resolved
reflectivity measurements, a white light source (Ocean Optics, HL-2000-FHSA)
was focused onto the sample by an infinity corrected ×100 nIR
objective with 0.85 NA (Olympus, LCPLN100XIR). The resulting spot
diameter of ∼2 μm defined the investigated area on the
sample. For angle-resolved PL, the white light source was replaced
with a 640 nm laser diode (Coherent OBIS, 5 mW, continuous wave) and
the reflected laser light was blocked by an 850 nm cutoff long-pass
filter. The reflected/emitted light from the sample was imaged onto
the entrance slit of an imaging spectrometer (Princeton Instruments
IsoPlane SCT 320) using a 4f Fourier imaging system (f1 = 200 mm and f2 = 300 mm).
The resulting angle-resolved spectra were recorded with a 640 ×
512 InGaAs array (Princeton Instruments, NIRvana:640ST). A linear
polarizer was placed in front of the spectrometer to select between
s and p polarization.
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5

Spectrophotometric Analysis of Herbicide Impacts

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Analysis of the effects of herbicides or inhibitors on the kinetics of charge recombination was performed using a Cary60 spectrophotometer connected to an external 1 cm cuvette holder (Ocean Optics) via a fibre-optic coupler. A white light pulse of 50 ms duration was applied to the sample cuvette at 90° to the pulsed measuring beam by an HL-2000-FHSA white light source with a fast shutter (Ocean Optics) delivering approximately 25 W m−2 illumination at the cuvette surface. The actinic pulse was triggered by a TGP110 pulse generator (Thurlby Thandur Instruments). Solutions of 13.2 µM reaction centres in 20 mM Tris (pH 8.0)/ 30 µM UQ0 were prepared with and without the addition of 500 µM atrazine, terbutryn, stigmatellin, bromoxynil, bentazon, capsaicin or DCMU. Test samples were loaded into to a 3×3 mm fluorescence cuvette (Hellma) aligned to the measuring and excitation pulses and absorbance at 865 nm was measured for 20 s after delivery of the light pulse, with a further period of at least 60 s to allow full dark adaptation of the reaction centres before re-excitation. A set of eight kinetic traces were recorded for each sample, averaged, and fitted using a single or double exponential function in Origin 8 (OriginLab).
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6

Electrochromic Behavior of Prussian Blue

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The
electrochromic behavior
of PB was studied using spectrochemistry in solution and a solid state
after electrodeposition on ITO-PET substrates. Samples were analyzed
using a spectrochemical setup including a halogen lamp (HL-2000-FHSA,
Ocean Optics) as a light source, a spectrophotometer (QE65000, Ocean
Optics), and a holder of the same branch for introducing the cuvette
with the sample, which ensures a fixed position for the optical fibers
and avoids the incidence of light during the measurement. As a cuvette,
a thin layer of quartz glass with two different optical paths from
BAS Inc. was used. A 1 cm optical path was employed to analyze PBSol samples in suspension. For PB-electrodeposited ITO-PET
electrodes, samples were analyzed directly after introduction into
the quartz cuvette cell and the optical path was 1 mm. Optical measurements
were acquired using a spectrophotometer and controlled by OceanView
software.
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7

Optical Sensing Substrate for PNRA Detection

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For the structure with PNRA on the quartz substrate, a home-build Polydimethylsiloxane (PDMS) flow cell is employed as holders of liquids solution before optical measurement. The flow cell is sandwiched between the sensing substrate and a PMMA plate. Inlet and outlet holes are drilled through PMMA plate to connect the tubing. All reflectance spectra on the quartz substrate are taken on a UV-Visible-NIR micro-spectrometer (PV20/30 from CRAIC Technologies). For the structure with PNRA on the tip of optical fiber, a home-built flow cell is used for injection and the ejection of sample solutions and the sufficient space for washing sensing surfaces. Light source, spectrometer and the fiber probe are connected by a binary beam fiber jumper. Light from a halogen lamp (HL-2000-FHSA, Ocean Optics, Inc.) is launched into one splitter end of the fiber jumper. The transmission spectrum is collected at the other splitter end of the fiber jumper through the spectrometer (HR4000, Ocean Optics, Inc.) and is displayed by a computer. The probe is mounted in the combined end of the fiber jumper. In the above optical measurement, a peristaltic pump is used to inject sample solutions with a constant flow rate of 0.2 ml/min.
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8

Characterization of a-Si:H Color Filters

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The completed a-Si:H pattern was visually evaluated under a high-resolution field emission scanning electron microscope (FESEM S-4800, Hitachi). The transmission spectra were examined for different polarizations by launching a collimated beam via a multimode fiber, which originates from a halogen lamp (HL-2000-FHSA, Ocean Optics) that is properly polarized via a calcite crystal polarizer (GTH 10M-A, Thorlabs), to the prepared filter that is mounted on a motorized rotation stage via a focusing lens. The optical output was captured by a spectrometer (Avaspec-3648, Avantes). The images relating to each pixel of the color filter were taken by a digital microscope (Leica DM4000 M).
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9

Spectral Irradiance Absorption in Nanofluids

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The spectral irradiance being absorbed by nanofluid is directly related to the photo-thermal conversion performance. The surfactant, ultrasonication time, and nanoparticle type can significantly impact the spectral irradiance being absorbed or transmitted through the nanofluid. The spectrophotometer (Ocean HDX, from Ocean Insight, USA) is used to measure the spectral irradiance ( μ W/cm2/nm) being transmitted through nanofluid in the mainly visible spectrum (400 – 800 nm). For the near-infrared region (900 – 2400 nm), the spectral irradiance transmitted was measured by spectrophotometer (NIR Quest, from Ocean Insight, USA). The halogen lamp (HL-2000-FHSA, from Ocean Insight, USA) was used as a light source during the experimentation.
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10

In Situ UV-Visible Spectroscopy for Coating

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In situ fast response ultraviolet (UV) visible absorption spectroscopy measurements were performed by the OCEAN-FX-VIS-NIR-ES spectrometer. The HL-2000-FHSA light source is purchased from Ocean Optics Inc. The spectrometer using the absorbance mode with the time resolution of 20 ms. The detector collects the absorbance spectra ranged from 400 to 1050 nm during coating. The instruments of ISFR-Abs experiment is displayed in fig. S14. There is a collimator in the “Y” shape optical fiber delivering incidence light and collecting reflecting light. The horizon position of the collimator can be tuned by a microcalliper, and the vertical position is fixed at 60 mm to substrate. The 60-mm distance is confirmed by a charge-coupled device (CCD), which can image the light spot. When the light spot meets minimum, the focal distance is 60 mm.
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