Presented by Peter De Wolf, Ph.D., Worldwide Application Director, Bruker Nano Surfaces and Metrology (December 7, 2022)
PRESENTATION HIGHLIGHTS:
[00:00:11] Measurements on cross-sectioned devices
[00:00:59] PiezoResponse Force Microscopy (PFM)
[00:03:17] Chemical property characterization by AFM-IR
[00:05:58] Other techniques for characterizing dielectric materials
Watch Now | 9 Minutes
Q&A
Presented by Peter De Wolf, Ph.D., Worldwide Application Director, Bruker Nano Surfaces and Metrology and Andrea Slade, Ph.D., Product Manager, Materials AFM, Bruker Nano Surface & Metrology (December 7, 2022)
PRESENTATION HIGHLIGHTS:
[00:00:00] What is the difference between C-AFM and TUNA and what is the maximum TUNA current?
[00:01:06] Can one get similar conductive AFM graphs on wide band gap semiconductors?
[00:01:48] How many I-V curves are recorded per pixel and is the I-V curve generated an average of multiple recordings?
[00:02:57] Are these kinds of conductivity measurements with TUNA also possible on materials that are less insulating or more bulky? (e.g., low band gap semiconductors, like silicon substrates or germanium)
[00:04:11] Is it possible to use KPFM to estimate the size of the depletion region in a PNP semiconductor device structure via the static charge distribution?
[00:05:51] What are the challenges for electrical measurements on softer samples and biological samples (e.g., neuronal cells that are also known to conduct electrical signals)?
[00:07:58] What materials can be detected by AFM-IR (on the Dimension IconIR system)?