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Newton du970n bv 353

Manufactured by Oxford Instruments
Sourced in United Kingdom

The Newton DU970N-BV-353 is a deep-cooled, back-illuminated, scientific CCD camera. It features a 1024 x 1024 pixel sensor with 13 x 13 μm pixel size. The camera offers a high quantum efficiency and low read noise, making it suitable for a variety of scientific applications.

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2 protocols using newton du970n bv 353

1

Confocal Raman Imaging of Nodule Structure

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Confocal Raman spectroscopy was performed using a 532-nm laser excitation Raman system (alpha300R+, WITec, Ulm, Germany). The z-stacked Raman images were acquired using a 63×/1.0 numerical aperture water immersion microscope objective lens (W Plan-Apochromat, Zeiss, Oberkochen, Germany). The scattered light was directed to the spectrometer via a 25-μm low OH silica fiber also acting as a pinhole that enables confocal imaging. A 600 groove/mm grating imaging spectrograph (UHTS 300, WITec, Ulm, Germany) was used, which allowed us to cover a spectral range of 0 to 3700 cm−1. Raman spectra were acquired using a thermoelectrically cooled back-illuminated charge-coupled device camera (Newton DU970N-BV-353, Andor, Belfast, UK). Each Raman spectrum was measured using 40-mW laser power at the sample with 0.2-s integration time. Imaging of the nodule was performed in “stack” mode by measuring 20 layers with 2-μm increments in the z direction spanning the entire nodule volume. Each x-y section of a Raman image covers ~160 μm by 120 μm, giving an overall spatial resolution of 2 μm.
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2

Raman Imaging of Cells on MgF2 Slides

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Magnesium fluoride (MgF 2 ) slides were pre-treated with BD Cell-Tak™ Cell and Tissue Adhesive in a 48-well tissue culture plate (BD Biosciences, 5.2 µL in 300 µL of sodium bicarbonate buffer, pH = 8 for 40 minutes at room temperature). Following two washing steps with ddH 2 O, MgF 2 slides were incubated with the cell suspension in PBS for 30 minutes. Slides were then fixed with 4% v/v PFA and washed gently with PBS before analysis. Raman spectral imaging was performed on a confocal Raman microscope (alpha300R+, WITec, Ulm, Germany). A 532 nm laser (Compass Sapphire, Coherent, Gottingen, Germany) was used for excitation. The laser beam was focused through a 63×/1.0 NA water immersion microscope objective lens (W Plan-Apochromat, Zeiss, Oberkochen, Germany). The Raman spectroscopy signals were dispersed by a grating (600 g mm -1 ) spectrograph (UHTS 300, WITec, Ulm, Germany) and the spectra acquired with a thermoelectrically cooled CCD detector (Newton DU970N-BV-353, Andor, Belfast, UK) with a spectral resolution of 3 cm -1 . Raman spectroscopy images ∼150 × 150 μm were produced with 400 nm spatial resolution, 1 s integration time and one accumulation per pixel. Spectral collection was centered at 2000 cm -1 (0-3000 cm -1 ). The Control FOUR software (version 4.0, WITec) was used for measurement and Project FOUR Plus (version 4.0, WITec) for spectral data processing.
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