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Ccd detector

Manufactured by Horiba
Sourced in Germany

The CCD detector is a type of image sensor that converts light into electrical signals, enabling the capture and recording of digital images. It plays a crucial role in various scientific and analytical instruments, including spectroscopy, microscopy, and astronomical imaging applications.

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6 protocols using ccd detector

1

Raman Spectroscopy Analysis of Samples

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Raman spectra were obtained using a HORIBA LabRAM HR Evolution equipped with a 532 nm laser. The Raman spectrometer is coupled to a CCD detector (Horiba) and a microscope equipped with a 100× magnification objective. A grating of 1800gr/mm was used to obtain high spectral resolution. For each sample, three spectra were recorded and averaged, peak area and maximum were determined by the application of a polynomial baseline and fitting with a Lorentzian function.
Spectra in the radial breathing mode (RBM) range were acquired with a 532 nm laser with 900 gr/mm, 100% ND filter, 10 s acquisition time and four accumulations in the range of 100 to 500 cm−1. From the mappings two representative spectra were selected for each sample.
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2

Raman Scattering Spectroscopy for Cell Analysis

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The SERS spectra were obtained using a single-stage spectrograph equipped with a CCD detector (Horiba, Munich, Germany) and a diode laser operated at 785 nm (Toptica, Graefelfing, Germany). To focus the excitation light and collect the Raman scattered light in 180 degree backscattering geometry, a 10× objective was used for the nanostar suspension samples and a 60× water immersion objective (N.A. 1.2) was used for the experiments with the culture media and the cells. The excitation intensity was 3 × 10 5 W cm -2 and 8 × 10 5 W cm -2 in these two experiments, respectively. All the spectra were obtained with an acquisition time of 1 s. Considering the whole recorded spectral range from 400 to 1800 cm -1 , the spectral resolution was 4-7 cm -1 . All spectrum pre-processing and band occurrence calculations were done using Matlab R2018a (The MathWorks, Inc.) and Wolfram Mathematica 12 software, respectively.
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3

SERS Spectroscopy for Cell Characterization

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SERS spectra were measured using a single-stage spectrograph equipped with a CCD detector (Horiba, Munich, Germany) and a diode operating at 785 nm (Toptica, Graefelfing, Germany), in a setup with a 180 degree backscattering geometry. A 60× water immersion objective (NA = 1.2) was used in the experiments with cells, and the excitation intensity on the samples was 8 × 105 W cm−2. All spectra were obtained with an acquisition time of 1 s, and the spectral resolution was 4–7 cm−1 considering the whole recorded spectral range (400–1800 cm−1). From 3T3 cells, 489 spectra from 15 cells were obtained for 3 h incubation with NS25, and 232 spectra were obtained from 6 cells for 6 h incubation. From HCT-116 cells, 100 spectra from 8 cells were measured for 3 h incubation with NS25, and 207 spectra were obtained from 7 cells for 6 h incubation. J774 cells spectra analysis was done with 370 spectra from 7 cells exposed to NS25, 252 spectra from 9 cells exposed to NS50, and 226 spectra from 10 cells exposed to NS75, all after an incubation time of 3 h. Processing of the spectra with Matlab R2018a (The MathWorks, Inc., Natick, MA, USA) included frequency calibration, baseline correction, and vector normalization. Band occurrence calculation was performed with Wolfram Mathematica 12 software.
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4

Resonance Raman Spectroscopy of MauG

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Resonance Raman spectra were recorded using a Raman spectrometer consisting of a Spex model 1877 triple spectrograph and a charge-coupled device (CCD) detector as reported previously [17 (link)]. A 406.7 nm line from an argon-krypton ion laser (Spectra-Physics BeamLok model 2080-KV) was used as the excitation source, and the Raman signal was collected in a 120° geometry. The laser power was adjusted to ~5 mW at the sample. Each spectrum was recorded with a 60 s accumulation time, and 10 repetitively measured spectra were averaged to improve the quality of the final spectrum. The frequencies of the Raman bands were calibrated using the standard spectrum of cyclohexane. Samples contained 0.2 mM MauG in 0.05 M phosphate buffer, pH 7.5, with 10% ethylene glycol either with or without 0.1 mM PreMADH. The ν3 bands were deconvoluted by the peak searching and fitting function of the LabSpec software provided with the CCD detector (Horiba Instruments) using a combination of the Gaussian and Lorentzian functions.
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5

Micro-Raman Characterization of Crustacean Eye

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Chemically fixed eyes of dark-adapted M. rosenbergii zoea 7 were cut into longitudinal sections (190 μm thick) using a vibratome. The preparation of the sections is described in the section 'TEM Imaging and electron diffraction on extracted particles'. The sections were placed on an aluminum metal disc. Spectra were obtained from the white. birefringent, reflective material in the eye. Micro-Raman measurements were performed with a confocal Horiba LabRam HR Evolution, equipped with a Syncerity CCD detector (deep-cooled to -60 ºC, 1024 x 256 pixels). The excitation source was a 633 nm laser, with a power (on sample) ranging from 1.2 to 3 mW. The laser was focused with a 60X water immersion objective (Olympus LUMPlanFLN 60XW, NA=1). The measurements were taken using a 600 g mm-1 grating and 80-100 μm confocal hole. Typical exposure times were 20 to 30 seconds, using 1 or 2 accumulations.
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6

Raman Spectroscopic Analysis of Tea Powder

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The appropriate quantity of tea powder was meticulously placed in the center of a spotlessly clean slide, and compressed using a cover slip. Raman spectra were subsequently acquired using an Xplora PLUS Raman spectrometer equipped with a CCD detector (HORIBA, France), as illustrated in Fig. 1 (b). The spectrometer parameters were set as follows: the numerical aperture of the 50× objective was 0.55NA, the laser wavelength was 785 nm (10% laser power, 3.6 mW), the objective lens was 50 times, the grating was 1200 gr/nm, the wavelength range spanned 100-3700 cm−1, the spectral resolution was 1.3 cm−1, and each Raman spectrum was scanned for a duration of 8 s. The environmental conditions during the collection of spectra were maintained at 23 °C with a relative humidity of 45%. Each sample was tested four times, with the sampling locations for each test being randomly selected.

Materials and environmental instruments: (a) Comparison of Baimudan tea from different producing areas; (b) the Xplora PLUS Raman spectrometer used in the experiment.

Fig. 1
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