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Hyperion 1000

Manufactured by Bruker
Sourced in United States

The Hyperion 1000 is a Fourier-transform infrared (FTIR) microscope system designed for materials analysis. The core function of the Hyperion 1000 is to enable high-resolution infrared imaging and spectroscopy of samples.

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11 protocols using hyperion 1000

1

Morphological Characterization of HSQ Microstructures

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The morphology and shape of HSQ microstructures constructed by FsLDW were measured by using field-emission scanning electron microscope (FE-SEM, S-4800, Hitachi) at 5 kV accelerating voltage after being deposited with a thin layer of Au. The surface roughness of the HSQ microstructures were measured using an atomic force microscope (AFM, Fastscan IconBio, Bruker). The optical microscopy images were characterized by a laser scanning confocal microscope (LSCM, A1R MP, Nikon) using an oil-immersion objective lens (N.A. = 1.40, 60 ×, Nikon). Raman and FT-IR spectra of HSQ film with and without fs laser exposure were characterized by using Raman spectroscopy (Raman-11, Nanophoton, excitation wavelength is 532 nm) and FT-IR spectroscopy (Vertex 70, Bruker) equipped with microscope (Hyperion 1000, Bruker). The reflectance spectra of the structural colour before and after thermal treatment were measured by using FT-IR spectroscopy (Vertex 70, Bruker) equipped with microscope (Hyperion 1000, Bruker). Structural colour of the HSQ microstructure was recorded by employing a charge coupled device (CCD) camera (Beijing Groupca Company) equipped on an optical microscope under reflection mode. The absorption spectrum of the HSQ film on quartz was recorded on a UV-Visible Spectrophotometer (UV-2550, Shimadzu).
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2

Infrared Spectroscopy of TP-β-CD Complex

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TP, β-CD and the TP-β-CD inclusion complex were obtained separately with IR grade potassium bromide at a ratio of 1:100, and IR pellets were prepared by applying 8 metric tonnes of pressure in a hydraulic press. The vibrational infrared spectra were measured between 500 and 4000 cm-1, with an FT-IR Bruker Equinox 55 spectrometer equipped with a Bruker Hyperion 1000 microscope. In order to analyze changes in the positions and intensity of bands in experimental spectra of the TP-β-CD inclusion complex, quantum-chemical calculations were performed based onB3LYP functional and 6-31G(d,p) as a basis set. All calculations were performed using the Gaussian 09 package and the GaussView application [21 ].
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3

Infrared Spectroscopic Analysis of RU-β-CD Inclusion Complex

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RU, β-CD andRU-β-CD inclusion complex co-grind mixture were obtained separately with IR grade KBr in the ratio of 1: 100, and corresponding pellets were prepared by applying 8 metric ton of pressure in hydraulic press. The vibrational infrared spectra were recorded between 400 and 5000 cm-1, with an FT-IR Bruker Equinox 55 spectrometer equipped with a Bruker Hyperion 1000 microscope. In order to analyse changes in positions and intensity in experimental spectra of RU-β-CD inclusion complex, quantum chemical calculations based on DFT were performed. All the calculations were made by using the Gaussian 03 package [18 ]. The GaussView application was utilized to propose the initial geometry of the investigated molecules and to visually inspect the normal modes.
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4

FTIR Spectroscopy Protocol

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The infrared absorption spectrum is measured by a Bruker Hyperion-1000 Fourier transform infrared spectrometer (FTIR).
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5

FTIR Analysis of Chemical Bonds

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Chemical bonds were analyzed by Fourier-transform infrared spectroscopy (FTIR), using a Hyperion 1000 spectrophotometer (Bruker, Santa Clara, CA, USA). The samples were placed in an ATR diamond sensor to obtain their infrared profile. The measurements were obtained between 4000 and 400 cm−1 with an opening of 4 cm−1 and an acquisition of 200 scans. Baseline correction was performed by measuring without a sample.
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6

Infrared Spectroscopy of Organic Compounds

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All compounds were obtained separately with IR grade potassium bromide at a ratio of 1:100, and IR pellets were prepared by applying 8 metric tons of pressure in a hydraulic press. The vibrational infrared spectra were measured between 4000 cm−1 and 4000 cm−1, with an FT-IR Bruker Equinox 55 spectrometer equipped with a Bruker Hyperion 1000 microscope. To analyze changes in the positions and intensity of bands in the experimental spectra of the systems, quantum-chemical calculations were performed based on B3LYP functional and 6-31G(d,p) as a basis set. All calculations were performed using the Gaussian 09 package and the GaussView application.
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7

Infrared Spectroscopy Analysis of CTZ-β-CD Complexation

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Infrared spectra for CTZ, β-CD, the CTZ–β-CD physical mixture and the CTZ–β-CD system were recorded with a Fourier transform infrared FT-IR Bruker Equinox 55 spectrometer equipped with a Bruker Hyperion 1000 microscope. All samples were measured in an absorption mode, in a frequency range of 400–2000 cm−1 and at a resolution of 4 cm−1. To analyze changes in positions and intensity in the experimental spectra of the CTZ–β-CD system, quantum chemical calculations based on DFT with B3LYP functional and 6-31G(d,p) basis set were conducted to obtain theoretical spectra of CTZ. The analysis of changes in experimental spectra and determination of binding domains of API in system was conducted according to theoretical spectrum of CTZ. All calculations were performed by using the Gaussian 09 package [32 ]. The scale factor applied to theoretical spectra was 0.964.
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8

Circular Polarized Light Detection Setup

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The detection setup schematic is shown in fig. S3B. The experimental setup consists of a reflection-based microscope (HYPERION 1000, Bruker Corp.) coupled to a FTIR spectroscopy system (VERTEX 80, Bruker Corp.). The spectrometer is configured with a MIR globar thermal source and a KBr beamsplitter. A broadband ZnSe linear polarizer (LP) with its fast axis along the horizontal direction is placed along the output of the FT-IR system’s beam path. The light is redirected toward a motorized rotation stage (PRM1Z8, Thorlabs)–mounted achromatic (4000 to 1429 cm−1) quarter-wave plate (QWP) (Bernhard Halle Nachfolger GmbH). The generated CPL is incident on the sensor surface, and the reflected response is redirected to a cryo-cooled MCT broadband infrared detector integrated within the microscope. The spectral response is measured for both right- and left-handed CPL excitation by rotation of the QWP to 45° and −45°, respectively, with respect to the LP axis. The final processing is performed with Bruker’s spectra measuring and processing software OPUS.
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9

Thermal Emissivity Measurement of Metamaterials

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Thermal emissivity of the metamaterial at 1,000 °C was obtained using a high-temperature heating stage (TS1500, Linkam) installed at the focus of the FTIR microscope (Bruker, Hyperion 1000) described previously. To calculate the emissivity, it was necessary to divide the thermal emission spectrum by the blackbody spectrum at the same temperature. This step also simultaneously eliminated any artifacts introduced by the setup from the emissivity measurement. As a reference, we replaced the sample with a glassy carbon SIGRADUR G substrate. At elevated temperatures, the glassy carbon is expected to have a wavelength independent emissivity varying between 0.87 and 0.9 in the infrared range.
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10

Spectroscopic Analysis of SUM Inclusion Complexes

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SUM and SUM-BCD and SUM-HPBCD inclusion complexes were obtained separately with IR grade potassium bromide at the ratio of 1:100, and IR pellets were prepared by applying 8 metric tons of pressure in a hydraulic press. The vibrational infrared spectra were measured between 500 and 1800 cm−1 with an FT-IR Bruker Equinox 55 spectrometer equipped with a Bruker Hyperion 1000 microscope. In order to analyze positions and intensity of bands in experimental spectra of SUM, quantum-chemical calculations were performed based on B3LYP functional and 6–31 G(d, p) as a basis set. All the calculations were made using the Gaussian 09 package and the GaussView application54 . While for prediction of the interactions of SUM and CD, theoretical research was conducted which presented the most provisional places of SUM inclusion into the cyclodextrin cavity.
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