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UHV Chamber

attoAFM-UHV

attoCFM-UHVs

Application Notes

 

 


attoRAMAN xs
low temperature confocal Raman microscope
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The attoRAMAN xs combines a high resolution, low temperature confocal microscope with ultra sensitive Raman optics. This innovative product enables state of the art confocal Raman measurements at cryogenic environments combined with magnetic fields of up to 15 T. It is a ready-to-use system and is delivered with Raman laser source (532 nm / 633 nm wavelength as excitation source available), ultra-high throughput spectrometer including a peltier-cooled, back-illuminated CCD, and a state-of-the-art Raman controller/software package.


Principle - Tha attoRAMAN uses free-beam optics to focus laser light onto a substrate. The reflected light is then collected by room temperature optics while the Rayleigh signal is being suppresed by a notch/edge filter. The remaining signal, containing the Raman information, is then guided into a highly sensitive spectrometer using a single- or multimode fiber (depening on the application). The spectrometer allows to analyze the wavenumber depenpdent Raman intensity with a resolution of up to 1 cm-1 as close as 100 wavenumbers to the Rayleigh line.


Objective Systems - attocube systems offers several low temperature confocal objectives which can be adjusted depending on your experimental requirements, the wavelength range, working distance, and other parameters. For customized solutions, please contact our office.


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Additional Information:
Available Controller for this Product:
ANC350 Piezo positioning controller for attocube's encoded positioners |
ANC300 Piezo positioning controller for attocube's open-loop positioners |

Complete System Solutions:
Complete system configurations for this product.







> true low temperature confocal Raman microscope
> modular beam splitter and filter optics at room temperature
> ultra-high transmission spectrometer and peltier-cooled back-illuminated CCD
> pixel resolution 1/cm at 1800/mm grating
> measurements as close as 100/cm to the Rayleigh line

> fits standard cryogenic and magnet sample spaces
> broad variety of applications ranging from simple 2D Raman images to Raman spectra along arbitrary 3D llines wihtin the sample
> excellent stability for long integration times and weakest signal detection
> highest measurement sensitivity
> access to a large area on the sample surface