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Dv401 bv

Manufactured by Oxford Instruments
Sourced in United Kingdom

The DV401-BV is a compact and versatile lab equipment product from Oxford Instruments. It is designed to provide accurate measurements and data analysis capabilities for various scientific applications. The core function of the DV401-BV is to perform high-precision data acquisition and processing tasks.

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5 protocols using dv401 bv

1

Micro-Raman Spectroscopy Protocol

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Raman spectroscopic analysis was performed with a CRM 300 WITec micro-Raman setup (WITec, Ulm) equipped with a 600 lines/mm grating. A frequency-doubled cw Nd-YAG laser beam with an excitation wavelength of 532 nm and a power of 15 mW before passing the objective was focused on the sample via a 60× Nikon water immersion objective with NA 1.0. The 180° backscattered light was detected by a back illuminated CCD camera (DV401 BV, Andor Technology Ltd, Belfast) with 1024 × 127 pixels cooled to −60°C.
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2

Raman Spectroscopy of Bacterial Samples

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Raman spectra were collected with a Raman microscope (BioParticle Explorer, rap.ID Particle Systems GmbH, Berlin, Germany). A solid-state frequency doubled Nd:Yag module (Cobolt Samba, 25 mW, Cobolt AB, Solna, Sweden) with an excitation wavelength of 532 nm was used. The laser light was focused through an 100x objective (Olympus MPlanFLN 100xBD) onto the sample. This result in a spot size <1 µm laterally so that approximately 7 mW hit the sample.The bacteria were measured from different regions of the specimens. The Rayleigh scattering was removed by two edge filters after collecting the 180°-backscattered light, while a thermoelectrically cooled CCD camera registered the light (Andor DV401-BV). A single-stage monochromator, consisting of a 920-line/mm grating, diffracted the backscattered light so that the spectral resolution accounted for about 8 cm−1. The integration time per Raman spectrum (15 to 3275 cm−1) was 5 seconds. Approximately 50 single-bacteria Raman spectra were measured per batch (biological replicate) and collected from four separately prepared batches for further analysis. The evaluation of the classification models was performed by using of about 20 spectra from other isolates (Table 2).
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3

Topography and Composition Analysis of CHO Cells

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The topography of the CHO cells was evaluated by AFM imaging, and measurements of the cells’ surface roughness were performed using the NT-MDT Solver system from NT-MDT Inc. in semi-contact mode using commercial silicon cantilevers with a tip diameter of 10 nm and force constant of 1.5 N/m. Cell surface roughness analysis was performed on the topography images of cell surface areas (5 × 5 µm) using Nova software from NT-MDT Inc. Surface roughness factors (10-point height (Sz) and average) were determined.
Energy-dispersive X-ray spectroscopy (EDS) analysis was performed to determine the TiO2-NPs content in CHO cells after exposure to the TiO2-NP colloidal solution. The samples were examined using a Hitachi S-3400N Type II scanning electron microscope (Tokyo, Japan).
The Raman spectra of CHO cells were registered using a confocal Raman system ‘upright INTEGRA Spectra’ from NT-MDT, using a 100× objective, 20 mW 532 nm wavelength DPSS laser, and a spectrometer—Solar TII from NT-MDT, equipped with a TE-cooled (−60 °C) CCD camera—DV401-BV from Andor Technology (Oxford Instruments, Abingdon, UK). The power of the laser at the sample was 0.4 mW, and the acquisition time was 20 s.
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4

Optical Characterization of GeOI Heterostructures

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A confocal multifunctional
microscope setup (Alpha300, WITec) equipped with a frequency doubled
Nd:YAG laser emitting linearly polarized light at λ = 532 nm
was employed for the optical characterization of the fabricated GeOI-based
Al-Ge-Al heterostructures. For confocal μ-Raman measurements,
a setup in backscattering geometry with a grating monochromator and
a CCD camera (DV401- BV, Andor) were used. For the PL measurements
in the near-infrared (NIR), a Princeton Instruments Acton SpectraPro
2300i spectrometer with a 150 g/mm grating (1.25 μm blaze wavelength),
300 mm focal length, and an Andor iDus DU491A-1.7 InGaAs detector
array was used. To avoid artifacts from VIS photoluminescence in NIR
spectra due to higher diffraction orders of the grating, an 800 nm
long-pass filter was put into the beam path. For both the μ-Raman
and the PL measurements, an achromatic Nikon EPI EPlan 100× objective
(NA = 0.9, WD = 0.23 mm), enabling a diffraction limited spot size
of ∼720 nm, was used.
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5

Multimodal Spectroscopic Analysis

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Raman spectra were collected using a confocal Raman microscope (a300; WITec) equipped with a CCD camera (DV401-BV; Andor), a Nikon objective (10Â) and a 532 nm laser (40 accumulations, integration time 1 s). Infrared spectra were recorded using a Thermo Scientific Nicolet is5 FTIR spectrometer (ATR-Diamond mode) (500 scans, resolution 2 cm À1 ).
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