IR-neaSCOPE
entry model for nanoscale IR imaging & spectroscopy
artefact-free absorption measurement
by decoupling efficiently optical from mechanical sample properties
maximum performance without sample damage
by accurate focusing of all illumination power onto the tip
high-quality results independent of user expertise
using intuitive software with a guided user interface
IR-neaSCOPE is designed for nanoscale analysis that only requires measurements of IR absorbtion. It detects laser-induced photothermal expansion in the sample using mechanical AFM-IR detection. Requiring no IR detector and interferometry, IR-neaSCOPE provides a cost-efficient solution most suitable for samples with large thermal expansion coefficients (e.g. polymers, biomaterials, etc.).
IR‑neaSCOPE delivers IR absorption imaging, point-spectroscopy and hyperspectral imaging. It is fully upgradable to IR‑neaSCOPE+s for advanced capabilities and access to a larger variety of sample material classes.
Customer Feedback
Edward Yoxall
Imperial College London, Department of Physics, London, UK
As a newcomer to the near-field optics I am very grateful for the prompt and competent support provided by neaspec’s experts.
Prof. Shinobu Hikami
Okinawa Institute of Science and Technology, Okinawa, Japan
The neaSCOPE new imaging technique offers me the right tool to unravel the fascinating world of protein folding in complex biological systems at the nanoscale.
Prof. Gerhard Ulm
Physikalisch Technische Bundesanstalt (PTB), Metrology Light Source (MLS), Berlin, Germany
Already after the first day of the system installation we have been able to measure publishable data.
Jaroslaw Syzdek, PhD
Lawrence Berkeley National Laboratory, Environmental Energy Technologies Division, Berkeley, USA
We were looking for a flexible research tool capable of characterizing our energy storage materials at the nanoscale. neaSCOPE proofed to be the system with the highest spatial resolution in infrared imaging and spectroscopy and brings us substantial new insights for our research.