
Since this step is very tedious, we tend to use an Arduino based exfoliation machine that peels the tape very slowly. Please ask a grad student if this is still operational.
Note: All acronyms of materials (ie: hBN = hexagonal boron nitride) are listed below in the section labeled Info on 2D materials. All temperatures are in Celsius.
Developing a plan in the form of a powerpoint is helpful – one can click the selection pane / name flakes / turn flakes on/off / adjust their transparency (in most ppt versions) to make visualizing the current transfer step easier.
To view a sample device plan go to the graphene network drive > Schaibley Lab > Wiki supplements and download the powerpoint labeled example of a device plan.pptx so that you can click around on the selection pane and transparency feature to see how useful these tools are.
Note the following terms to be used in this guide

Note the knobs on the micromanipulator

Using two microscope objectives during the transfer is good enough because the digital zoom on the canon software is available, so this gives you 4 zoom levels.
The best way to get good at transferring is to do many transfers. Beginner tip: start simple – try to pick up graphene with hBN, or make it a little more difficult and completely encapsulate a flake (could be graphene again) between two hBN pieces. Transferring with expendable flakes reduces beginner anxiety and allows one to gain confidence in the process.


You have the least probability of tearing the graphene strip if you make the stamp “flow” in a certain direction.

The idea is that when the cooldown sequence occurs and the PC begins to “roll back” to its original position, that there are no competing forces pulling on the thin graphene. The vdW force between the hBN/graphene and then the force between the PC/graphene occur – one and then the other instead of both simultaneously which would increase the likelihood of ripping the graphene.
You also want to consider any dirt on your stamp/chip and try to avoid it. Remember these flakes are very small comparatively so if there is dirt nearby the flake a “tent” of PC might form and you may be unable to touch the flake of interest with the stamp. Gently dust the chip with N2 before transferring. The good news is that you only need a relatively small portion of your stamp to be pristine in order to build a nanostructure.

Note in the above picture that there are dotted and solid perimeters outlined. This author uses dotted perimeters as a signal to himself that this flake/bulk has been very carefully traced and the marks can be trusted more than the solidly outlined landmarks. Again, this whole process is a balance act. The more landmarks you outline the better (after all, some won’t pick up), but you don’t have to painstakingly trace each one. 2-3 with dotted perimeters will do (including the main flake on all 4 zoom levels), then quickly trace a couple more bulk pieces.
Another quick adam trick: one digital level =live at one time
[need picture of labview UI]

WSe2 is a transition metal dichalcogenide which, in monolayer form, has a direct band-gap of 1.7eV (~730nm). One can confirm the existence of a monolayer of WSe2 by collecting photoluminescence produced by electron/hole recombination with a spectrometer, because WSe2 consisting of >1 layers will have an indirect band-gap and the electron/hole recombination processes will not be predominantly optical.
Show a monolayer of WSe2. Also show its band structure and maybe a 3d cartoon

WSe2 PL spectrum here

WSe2 is a transition metal dichalcogenide which, in monolayer form, has a direct band-gap of 1.7eV (~730nm). One can confirm the existence of a monolayer of WSe2 by collecting photoluminescence produced by electron/hole recombination with a spectrometer, because WSe2 consisting of >1 layers will have an indirect band-gap and the electron/hole recombination processes will not be predominantly optical.
Show a monolayer of WSe2. Also show its band structure and maybe a 3d cartoon

WSe2 PL spectrum here

WSe2 is a transition metal dichalcogenide which, in monolayer form, has a direct band-gap of 1.7eV (~730nm).

WSe2 PL spectrum here, both RT and cold.
Also put band structure

WSe2 is a transition metal dichalcogenide which, in monolayer form, has a direct band-gap of 1.7eV (~730nm). One can confirm the existence of a monolayer of WSe2 by collecting photoluminescence produced by electron/hole recombination with a spectrometer, because WSe2 consisting of >1 layers will have an indirect band-gap and the electron/hole recombination processes will not be predominantly optical.
Show a monolayer of WSe2. Also show its band structure and maybe a 3d cartoon

WSe2 PL spectrum here

WSe2 is a transition metal dichalcogenide which, in monolayer form, has a direct band-gap of 1.7eV (~730nm). One can confirm the existence of a monolayer of WSe2 by collecting photoluminescence produced by electron/hole recombination with a spectrometer, because WSe2 consisting of >1 layers will have an indirect band-gap and the electron/hole recombination processes will not be predominantly optical.
Show a monolayer of WSe2. Also show its band structure and maybe a 3d cartoon

WSe2 PL spectrum here

FePS3 is a transition metal thiophosphate which exhibits out-of-plane, long range anti-ferromagnetic ordering below T_N=123K where T_N is called the Neel temperature. [1]
Here’s a slide from the following pdf that highlights exfoliation and characterization of FePS3 in the glovebox. [maybe enter some stuff about the crystal structure, such as a 3d cartoon]
