The largest database of trusted experimental protocols

Liquid nitrogen cooledccd detector

Manufactured by Horiba
Sourced in United States

The Liquid-nitrogen-cooled CCD detector is a specialized laboratory instrument designed for high-sensitivity optical detection. It utilizes a charge-coupled device (CCD) sensor that is cooled with liquid nitrogen to reduce thermal noise and improve the signal-to-noise ratio. This device is primarily used for applications requiring low-light detection, such as spectroscopy, astronomy, and other scientific research.

Automatically generated - may contain errors

3 protocols using liquid nitrogen cooledccd detector

1

Raman Spectroscopy of Liposome Suspensions

Check if the same lab product or an alternative is used in the 5 most similar protocols
The Raman spectra were excited by
a 785 nm diode laser (Toptica, Munich, Germany) using an intensity
of 3.5 × 105 W cm–2 yielded when
focusing the excitation light with a 60× water immersion objective
into a droplet of liposome suspension. Raman light was directed to
a single-stage spectrograph equipped with a liquid-nitrogen-cooled
CCD detector (Horiba, Munich, Germany). The spectral resolution is
∼2 cm–1 considering the full spectral range
of 300–1900 cm–1. From each sample, a series
of 300 spectra was collected using an acquisition time of 1 s per
spectrum. The spectra were frequency-calibrated using a spectrum of
a toluene–acetonitrile mixture (1:1).
Preprocessing of
the spectra comprised removal of spikes, background correction using
asymmetric least-squares (AsLS) algorithm,44 (link) and vector-normalization in MatLab R2020b (The MathWorks, Inc.).
After removal of spectra with no signal, there were 98, 136, and 174
spectra remaining for the PA/PC/CER, PA/PC, and CER samples, respectively.
The remaining 98 spectra of PA/PC/CER in a range of 500–1700
cm–1 were subjected to hierarchical cluster analysis
(HCA) using SPSS 20 software (IBM Corporation, Armonk, NY). Band occurrences
in all individual spectra were analyzed using a script in Mathematica
12.1 (Wolfram) as detailed in ref (45 (link)). Average spectra of each HCA class were calculated
for further qualitative analysis of SERS signals.
+ Open protocol
+ Expand
2

Spectroscopic Analysis of DyP Peroxidases

Check if the same lab product or an alternative is used in the 5 most similar protocols
UV-Visible and RR experiments were performed using 2–4 μM and 150–300 μM DrDyP or DrDyPM190G, respectively, in 40 mM Britton–Robinson (BR) buffers at different pH values (3–10). UV-Visible spectra were recorded using a Shimadzu UV-1800 spectrophotometer (Shimadzu, Kyoto, Japan) with a temperature-control module set to 18 °C. Formation of DrDyP reaction intermediates was monitored after the addition of excess H2O2 (0.04–4 mM) to the protein solutions. RR solution measurements were completed at room temperature (RT) with 413 nm excitation source. A rotating quartz cell (Hellma, Müllheim, Germany) containing ca. 90 μL of sample was used in all measurements. The spectra were collected in backscattering geometry using a confocal microscope equipped with an Olympus 20× objective (working distance of 21 mm, numeric aperture of 0.35). The microscope was coupled to a Raman spectrometer (Jobin Yvon U1000, Edison, NJ, USA) with a 1200 lines/mm grating and a liquid-nitrogen-cooled CCD detector (Horiba). The laser beam was focused onto the sample with a power of 1.5–3.0 mW and 40–60 s accumulation time. Typically, 4–10 spectra were co-added in each measurement to improve signal-to-noise ratio. RR spectra were subjected to polynomial baseline subtraction and component analysis as described previously [33 (link)].
+ Open protocol
+ Expand
3

Raman Spectroscopy of Aqueous Solutions

Check if the same lab product or an alternative is used in the 5 most similar protocols
Raman spectra were collected for aqueous solutions in the range of 0.0 r h r 2.5. Measurements were performed with a LabRam HR800 spectrometer (Horiba Jobin Yvon, Bensheim, Germany), equipped with a 633 nm HeNe laser (Horiba Jobin Yvon, Bensheim, Germany), a 300 lines per mm grating, and a BX41 microscope (Olympus, Hamburg, Germany). The backscattered Raman light was collected by a liquid nitrogen-cooled CCD detector (1024 Â 256 pixels, Horiba). Using a 60Â immersion objective, the laser intensity at the liquid sample was 5.09 Â 10 5 W cm À2 . Reported Raman spectra are averages of five sweeps, each recorded with an acquisition time of 10 s. All measurements were performed 1 h after solution preparation.
+ Open protocol
+ Expand

About PubCompare

Our mission is to provide scientists with the largest repository of trustworthy protocols and intelligent analytical tools, thereby offering them extensive information to design robust protocols aimed at minimizing the risk of failures.

We believe that the most crucial aspect is to grant scientists access to a wide range of reliable sources and new useful tools that surpass human capabilities.

However, we trust in allowing scientists to determine how to construct their own protocols based on this information, as they are the experts in their field.

Ready to get started?

Sign up for free.
Registration takes 20 seconds.
Available from any computer
No download required

Sign up now

Revolutionizing how scientists
search and build protocols!