{"id":117,"date":"2023-10-24T07:33:28","date_gmt":"2023-10-24T07:33:28","guid":{"rendered":"https:\/\/flats.c2n.universite-paris-saclay.fr\/?page_id=117"},"modified":"2024-09-22T16:25:06","modified_gmt":"2024-09-22T16:25:06","slug":"stacking-twisting","status":"publish","type":"page","link":"https:\/\/newflats.c2n.universite-paris-saclay.fr\/?page_id=117","title":{"rendered":"Stacking &#038; Twisting"},"content":{"rendered":"\n<p><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-luminous-vivid-orange-color\">Our experts:<\/mark><\/strong> <a href=\"J.Diez@lmu.de\" data-type=\"link\" data-id=\"J.Diez@lmu.de\">Jaime Diez Merida<\/a> (LMU), <a href=\"Dmitri.Efetov@lmu.de\" data-type=\"link\" data-id=\"Dmitri.Efetov@lmu.de\">Dmitri Efetov<\/a> (LMU), <a href=\"maelle.kapfer@c2n.upsaclay.fr\" data-type=\"link\" data-id=\"maelle.kapfer@c2n.upsaclay.fr\">Maelle Kapfer<\/a> (UPSaclay), <a href=\"gaia.maffione@c2n.upsaclay.fr\">Gaia Maffione <\/a>(UPSaclay) and <a href=\"rebeca.ribeiro-palau@cnrs.fr\">Rebeca Ribeiro-Palau<\/a> (CNRS)<\/p>\n\n\n\n<p>Clean exfoliated 2D materials are the first step to a great van der Waals heterostructure. There are many tricks to it but the real way to do a great exfoliation is experience! Of course the right type of tape and a clean substrate also help.<\/p>\n\n\n\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"259\" src=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2023\/10\/Exfoliation_materials-1-1024x259.png\" alt=\"\" class=\"wp-image-140\" srcset=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2023\/10\/Exfoliation_materials-1-1024x259.png 1024w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2023\/10\/Exfoliation_materials-1-300x76.png 300w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2023\/10\/Exfoliation_materials-1-768x194.png 768w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2023\/10\/Exfoliation_materials-1-1536x388.png 1536w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2023\/10\/Exfoliation_materials-1-2048x517.png 2048w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><figcaption class=\"wp-element-caption\"><strong>Exfoliation of BN, graphene and graphite, respectively from left to right, on a Si substrate with 285 nm of <strong>thermally grown SiO<sub>2<\/sub><\/strong>.<\/strong><\/figcaption><\/figure>\n\n\n\n<p class=\"has-text-align-left\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-vivid-cyan-blue-color\">Choose your tape:<\/mark> <\/strong>This is a long lasting controversy since many research groups use blue clean room tape and others regular scotch tape. There is not major difference between these two since most of the research groups are able to obtain clean flakes but here once again you should make your own experience and try different tapes since the results can vary depending on the humidity and temperature of the room where you are exfoliating.<\/p>\n\n\n\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"415\" src=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2023\/12\/image-1024x415.png\" alt=\"\" class=\"wp-image-144\" srcset=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2023\/12\/image-1024x415.png 1024w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2023\/12\/image-300x122.png 300w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2023\/12\/image-768x312.png 768w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2023\/12\/image.png 1215w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><figcaption class=\"wp-element-caption\"><strong>Photograph of the varieties of tape available. Nitto tapes (A) ELP BT-130E-SL (B) ELPBT-150E-KLand (C )ELPBT-50E-FR along side Ultron tapes (D)1007R-6.0 and (E) 1009R-6.0. Adapted from<a href=\"https:\/\/research.manchester.ac.uk\/en\/studentTheses\/fabrication-and-optical-studies-of-air-sensitive-two-dimensional-\" data-type=\"link\" data-id=\"https:\/\/research.manchester.ac.uk\/en\/studentTheses\/fabrication-and-optical-studies-of-air-sensitive-two-dimensional-\"> Daniel Terry&#8217;s PhD thesis<\/a><\/strong><\/figcaption><\/figure>\n\n\n\n<p><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-vivid-cyan-blue-color\">Heating technique:<\/mark><\/strong> in order to obtain large area monolayer and bilayer graphene and other 2D materials it is highly recommended to use the technique developed in <a href=\"https:\/\/pubs.acs.org\/doi\/10.1021\/acsnano.5b04258\" data-type=\"link\" data-id=\"https:\/\/pubs.acs.org\/doi\/10.1021\/acsnano.5b04258\">this article<\/a>. In short, you will need to clean your Si\/SiO<sub>2<\/sub> chips in a soft oxygen plasma before approaching the tape with your exfoliated material, once in contact you will need to heat them up in a hot plate at ~100 <sup>o<\/sup>C for about 2 minutes, let them cool down after and pill off the tape.<\/p>\n\n\n\n<p><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-vivid-cyan-blue-color\">BN exfoliation: <\/mark><\/strong>for BN exfolaition (not too thin flakes) the process is the same but without heating the substrate before pilling off the tape. Avoiding heating leave cleaner flakes in the case of BN.<\/p>\n\n\n\n<p><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-vivid-purple-color\">Pro-tips: <\/mark><\/strong><\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li>Make sure, if you are using a RIE, that the plasma is not too strong and don&#8217;t do it for long, we normally use 20-30 s, otherwise the pickup becomes very difficult.<\/li>\n\n\n\n<li>Press gently with your tumb the tape while the chips are in the hot plate to get a better contact of the exfoliated material with the tape.<\/li>\n<\/ul>\n\n\n\n<p><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-vivid-cyan-blue-color\"><strong>Identifying the number of layers:<\/strong> <\/mark>Following the exfoliation process, the number of layers on a flake can be identified using their optical contrast with the substrate when observing with an optical microscope. The amplitude of the contrast will depend on the material (graphene, BN\u2026), the substrate (for example thickness of SiO2) and the wavelength of the illuminating light [<a href=\"https:\/\/arxiv.org\/abs\/0705.0259\">reference article<\/a>]. When high enough, the contrast will present discrete steps whose amplitude is directly linked to the number of layers.<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"643\" height=\"534\" src=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/Screenshot-2024-07-23-at-17.13.01.png\" alt=\"\" class=\"wp-image-404\" srcset=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/Screenshot-2024-07-23-at-17.13.01.png 643w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/Screenshot-2024-07-23-at-17.13.01-300x249.png 300w\" sizes=\"auto, (max-width: 643px) 100vw, 643px\" \/><figcaption class=\"wp-element-caption\">Optical image of graphite exfoliated on a 285 nm thick SiO2 layer. The different thicknesses can be identified by optical contrast.<\/figcaption><\/figure><\/div>\n\n\n<p><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-vivid-purple-color\"><strong>Pro tips:<\/strong><\/mark><\/p>\n\n\n\n<p>You quantify the contrast of a monolayer of your material by using a software like <a href=\"https:\/\/imagej.net\/ij\/\">ImageJ<\/a>. For this split the channels by color (Red, Blue, Green) and trace a line covering different thicknesses and extract the monolayer thickness.<\/p>\n\n\n\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"395\" src=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/Screenshot-2024-07-23-at-17.40.31-1024x395.png\" alt=\"\" class=\"wp-image-411\" srcset=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/Screenshot-2024-07-23-at-17.40.31-1024x395.png 1024w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/Screenshot-2024-07-23-at-17.40.31-300x116.png 300w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/Screenshot-2024-07-23-at-17.40.31-768x297.png 768w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/Screenshot-2024-07-23-at-17.40.31.png 1401w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n\n\n\n<p>Additionally, Atomic Force Microscopy (AFM) topography can be combined with the optical contrast to determine the number of layers on a flake. This is especially helpful when characterizing a new material whose contrast with the substrate is unknown.<\/p>\n\n\n\n<p>Finally, Raman spectroscopy can be particularly useful to identify monolayers [<a href=\"https:\/\/www.sciencedirect.com\/science\/article\/abs\/pii\/S0370157309000520\">reference article<\/a>].<\/p>\n\n\n\n<p>While contrast is a powerful and most notably fast way of identifying layer number, it tends to saturate for high number of layers where AFM topography will give the exact thickness of the flake.<\/p>\n\n\n\n<p>Lastly in some cases, given any combination of substrate and light wavelength, the optical contrast can remain low, this is for example the case of monolayer BN, and other methods are necessary to identify monolayers.<\/p>\n\n\n\n<p><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-vivid-cyan-blue-color\">Particularly hard to find, monolayer BN<\/mark><\/strong>: monolayer and thin BN are specially difficult to obtain and to find with an optical microscope. In our experience (and already documented in the literature here), the best way to obtain monolayer graphene is by using the heating technique explained before. Doing this in a 90 nm SiO2 layer will allow you to have enough contrast to see the monolayers, to improve their visibility you can use a U-DICR polarizer. <\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"701\" height=\"313\" src=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/image.png\" alt=\"\" class=\"wp-image-408\" srcset=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/image.png 701w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/image-300x134.png 300w\" sizes=\"auto, (max-width: 701px) 100vw, 701px\" \/><figcaption class=\"wp-element-caption\">Optical microscope image of monolayer BN exfoliated on a 90 nm SiO2 layer. (Left) unpolarized light. (Right) polarized light.<\/figcaption><\/figure><\/div>\n\n\n<h2 class=\"wp-block-heading\"><strong>Stacking of 2D materials:<\/strong><\/h2>\n\n\n\n<p>Before starting to stack your 2D materials you should think in what type of stack you want to do and what are the more appropriated methods to do so. Here are some examples:<\/p>\n\n\n\n<p><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-vivid-cyan-blue-color\">Stacking to a fragile substrate (e.g., TEM grid):<\/mark><\/strong> For this you migth want to use the membrane transfer. This one consist in exfoliating in a polymer and releasing this as a membrane to later deposit it the target substrate. You can find all the details in this <a href=\"https:\/\/pubs-acs-org.inp.bib.cnrs.fr\/doi\/10.1021\/nl5006542\" data-type=\"link\" data-id=\"https:\/\/pubs-acs-org.inp.bib.cnrs.fr\/doi\/10.1021\/nl5006542\">article<\/a> and its supplementary.<\/p>\n\n\n\n<p><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-vivid-cyan-blue-color\">Stamping:<\/mark><\/strong> This is the so called dry technique and consists in using a 2D material to pick up sucesive 2D materials. One of the first publications to explain the technique is <a href=\"http:\/\/10.1126\/science.124435\">here<\/a>. The animation below is very self-explanatory of the process.<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"480\" height=\"270\" src=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/pickup_CD.gif\" alt=\"\" class=\"wp-image-252\"\/><figcaption class=\"wp-element-caption\"><strong>Illustration of the principle of stacking 2D materials process. Courtesy of Cory Dean (Columbia University).<\/strong><\/figcaption><\/figure><\/div>\n\n\n<p>The process consist in picking up the different 2D materials one at the time using a combination of polymers (<em>e.g.<\/em>, PPC or PC on top of PDMS). After picking up all the different 2D materials the polymer is melted on top and the stack deposited on the substrate of your preference.<\/p>\n\n\n\n<p><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-vivid-cyan-blue-color\">The hot pick up technique<\/mark> (under construction)<\/strong>:<\/p>\n\n\n\n<p><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-vivid-cyan-blue-color\">Bubble squeezing: <\/mark><\/strong>After picking up all the layers you might realize that some bubbles are formed in your stack. This are formed of tape residues, water and\/or air. To clean up your stack you can squeeze the bubbles mechanically at higher temperatures. The techniques to do this (either with PC or PPC) are described in the following <a href=\"https:\/\/www.nature.com\/articles\/s41467-018-07558-3\">article<\/a>. As you can see in the pictures bellow the technique is very effective to get ride of bubbles<\/p>\n\n\n\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-9d6595d7 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<figure class=\"wp-block-image size-full is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"585\" height=\"442\" src=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/Bubble_1-2.png\" alt=\"\" class=\"wp-image-328\" style=\"width:416px;height:auto\" srcset=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/Bubble_1-2.png 585w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/Bubble_1-2-300x227.png 300w\" sizes=\"auto, (max-width: 585px) 100vw, 585px\" \/><figcaption class=\"wp-element-caption\"><strong>Stack on PPC slide before bubbles squeezing<\/strong><\/figcaption><\/figure>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\">\n<figure class=\"wp-block-image size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"580\" height=\"436\" src=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/Bubble_2-1.png\" alt=\"\" class=\"wp-image-329\" srcset=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/Bubble_2-1.png 580w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/Bubble_2-1-300x226.png 300w\" sizes=\"auto, (max-width: 580px) 100vw, 580px\" \/><figcaption class=\"wp-element-caption\"><strong>Squeezing process in progress<\/strong><\/figcaption><\/figure>\n<\/div>\n<\/div>\n\n\n\n<p><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-vivid-cyan-blue-color\">PDMS stamping:<\/mark><\/strong> As you could see all along this post we have mentioned two main polymers PC and PPC that are deposited on top of PDMS, these are the most used ones in for the stacking. However, there are other polymers also used for this, in the following table we summarize them and give you their main use and temeprature range to be used.<\/p>\n\n\n\n<figure class=\"wp-block-table\"><table><tbody><tr><td><strong>Polymer<\/strong><\/td><td><strong>Temperature <\/strong><br><strong>pick-up<\/strong><\/td><td><strong>Temperature release<\/strong><\/td><td>Cleaning<\/td><\/tr><tr><td>PPC <br>Ploy(propylene carbonate)<\/td><td>40 <sup>o<\/sup>C<\/td><td>80 <sup>o<\/sup>C \u2013 120 <sup>o<\/sup>C<\/td><td>Annealing in vacuum <br>at 360 <sup>o<\/sup>C<\/td><\/tr><tr><td>PC <br>Polycarbonate<\/td><td>80 <sup>o<\/sup>C<\/td><td>180 <sup>o<\/sup>C<\/td><td>Chloroform<\/td><\/tr><tr><td>PET <br>Poly(ethylene terephthalate)<\/td><td>60 <sup>o<\/sup>C<\/td><td>130 <sup>o<\/sup>C<\/td><td><\/td><\/tr><tr><td>PVC <br>Poly(vinyl choride)<\/td><td>70 <sup>o<\/sup>C<\/td><td>130 <sup>o<\/sup>C<\/td><td><\/td><\/tr><tr><td>PCL<br>Poly(caproalactone)<\/td><td>30 <sup>o<\/sup>C<\/td><td>60 <sup>o<\/sup>C<\/td><td><\/td><\/tr><\/tbody><\/table><figcaption class=\"wp-element-caption\"><strong>Table of polymers to transfer 2D materials in a PDMS stamp<\/strong><\/figcaption><\/figure>\n\n\n\n<h2 class=\"wp-block-heading\"><strong>TWISTING!<\/strong><\/h2>\n\n\n\n<p>Now that you have the basic notions of stacking you can start preparing twisting heterostructures. For twisted graphene structures the most widely used technique is the tear and stack technique detailed <a href=\"http:\/\/dx.doi.org\/10.1021\/acs.nanolett.5b05263\">here<\/a>. However, the tear part of this technique has been proven to give many problems of breakign the layers. A clear improvement in reproducibility has come with the implementation of different techniques to cut graphene before starting the stacking. Here we list few of them:<\/p>\n\n\n\n<ul class=\"wp-block-list\">\n<li><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-vivid-cyan-blue-color\"><strong>AFM cutting:<\/strong> <\/mark>the anodic oxidation nanolithography consist in applying a high frequency (&gt;10 kHz) AC voltage to a Pt\/Ir coated AFM tip (e.g., Arrow-NCPt-50, available <a href=\"https:\/\/www.nanoandmore.com\/AFM-Probe-ARROW-NCPt\">here<\/a>), to design on it a desired pattern, the resolution of the cut can go down to 10 nm, which makes it particularly interesting for polymer-free lithography of graphene. The full explaination can be found in this research <a href=\"https:\/\/doi-org.ezproxy.universite-paris-saclay.fr\/10.1021\/acs.nanolett.8b04166\">article<\/a>. An example of what can be done in graphene:<\/li>\n<\/ul>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"626\" height=\"808\" src=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/image-7.png\" alt=\"\" class=\"wp-image-260\" style=\"width:238px;height:auto\" srcset=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/image-7.png 626w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/image-7-232x300.png 232w\" sizes=\"auto, (max-width: 626px) 100vw, 626px\" \/><figcaption class=\"wp-element-caption\"><strong>Optical image of a graphene sheet cuted with an AFM.<\/strong><\/figcaption><\/figure><\/div>\n\n\n<ul class=\"wp-block-list\">\n<li><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-vivid-cyan-blue-color\">AFM tip on PDMS cutting:<\/mark><\/strong> A cheaper version of this technique can be achieved by sticking an AFM tip to a PDMS stamp. The PDMS stamp is placed in a transfer station, the optical microscope of this allows you to see when the tip enters in contact by a change in its reflectance. Once in contact the stage is moved to cut the graphene or move pieces of 2D materials that you don&#8217;t want in the way, as depicted in the picture below.<\/li>\n<\/ul>\n\n\n\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"590\" src=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/Open-JaimeDiez_Thesis-2-1024x590.jpeg\" alt=\"\" class=\"wp-image-337\" srcset=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/Open-JaimeDiez_Thesis-2-1024x590.jpeg 1024w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/Open-JaimeDiez_Thesis-2-300x173.jpeg 300w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/Open-JaimeDiez_Thesis-2-768x443.jpeg 768w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/Open-JaimeDiez_Thesis-2-1536x885.jpeg 1536w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/Open-JaimeDiez_Thesis-2.jpeg 1801w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><figcaption class=\"wp-element-caption\"><strong>a, AFM tip on PDMS stamp. b, AFM tip cutting a graphene flake, zoom on the flake after cut can be seen in c. d-f, AFM tip use to remove an undesirable BN flake<\/strong><\/figcaption><\/figure>\n\n\n\n<ul class=\"wp-block-list\">\n<li><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-vivid-cyan-blue-color\">Laser cutting:<\/mark><\/strong> by using a laser (filters between 500 nm and 600 nm) we can perform cuts in graphene and graphite layers in a fast and easy way. This technique was developed by Lutz Waldecker at RWTH and we added a joystick to to make it easier to use:<\/li>\n<\/ul>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"452\" height=\"452\" src=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/Laser_cut.gif\" alt=\"\" class=\"wp-image-267\"\/><figcaption class=\"wp-element-caption\"><strong>Laser cutting in action. You can see as the laser spot cuts a thick piece of graphite leaving a trench os ~4 um.<\/strong><\/figcaption><\/figure><\/div>\n\n\n<h2 class=\"wp-block-heading\"><strong>Rotatable structures<\/strong><\/h2>\n\n\n\n<p>The techniaues presented before are useful to build static angle van der Waals heterostructures, however, it is possible to control the angle dynamically. This will allow to investigate the evolution of the properties if a heterostructure as a function of the twist angle. Although the twisted bilayer version of this technique is still under development by our consortium, in this <a href=\"https:\/\/doi-org.inp.bib.cnrs.fr\/10.1126\/science.aat6981\">article<\/a> you can find the decription of the technique applied to graphene\/BN twisted structures.<\/p>\n\n\n\n<div class=\"wp-block-group\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-9d6595d7 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:100%\">\n<div class=\"wp-block-group is-nowrap is-layout-flex wp-container-core-group-is-layout-ad2f72ca wp-block-group-is-layout-flex\">\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"616\" src=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/image-14-1024x616.png\" alt=\"\" class=\"wp-image-286\" srcset=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/image-14-1024x616.png 1024w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/image-14-300x180.png 300w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/image-14-768x462.png 768w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/image-14-1536x924.png 1536w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/image-14.png 2034w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n\n\n\n<figure class=\"wp-block-image size-full\"><img loading=\"lazy\" decoding=\"async\" width=\"880\" height=\"720\" src=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/05\/Rotating_Handle.gif\" alt=\"\" class=\"wp-image-278\"\/><\/figure>\n<\/div>\n<\/div>\n<\/div>\n<\/div><\/div>\n\n\n\n<h2 class=\"wp-block-heading\"><strong>Imaging moire superlattices<\/strong><\/h2>\n\n\n\n<p>When fabricating twisted heterostructures it is essential to be able to characterize the twist angle throughout the stacking process. Currently AFM imaging techniques are being used. While some techniques offer high contrast between moir\u00e9 domains for a wide range of materials and twist angles such as conducting AFM (<a href=\"https:\/\/doi.org\/10.1038\/nphys2954\">reference<\/a> and <a href=\"https:\/\/arxiv.org\/abs\/1401.2637\">ArXiv<\/a>) and Scanning Microwave Impedance Microscopy (<a href=\"https:\/\/pubs-acs-org.inp.bib.cnrs.fr\/doi\/full\/10.1021\/acs.nanolett.1c00601\">reference<\/a>) those either require an electrical contact to the heterostructure or specialized equipment.<\/p>\n\n\n\n<p>Contact mode imaging is then the ideal way to image moir\u00e9 as no electrical contact is required and can be done either on when the stack is on a SiO<sub>2<\/sub> chip (left picture) or directly on the PDMS stamp used for stacking (right picture). Techniques such as Piezo-Force Microscopy [<a href=\"https:\/\/www.nature.com\/articles\/s41565-020-0708-3\">reference<\/a>], Lateral Force Microscopy (LFM) and Torsional Force Microscopy (TFM) [<a href=\"https:\/\/www.pnas.org\/doi\/10.1073\/pnas.2314083121\">reference<\/a>] will give high contrast between moir\u00e9 domains depending on the tip used (soft for LFM for example) and the normal force applied on the twisted structure (high for TFM).<\/p>\n\n\n\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-9d6595d7 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:100%\">\n<figure class=\"wp-block-gallery has-nested-images columns-default is-cropped wp-block-gallery-1 is-layout-flex wp-block-gallery-is-layout-flex\">\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"1024\" data-id=\"395\" src=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/moire_graphene_on_bn_small-2-1024x1024.png\" alt=\"\" class=\"wp-image-395\" srcset=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/moire_graphene_on_bn_small-2-1024x1024.png 1024w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/moire_graphene_on_bn_small-2-300x300.png 300w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/moire_graphene_on_bn_small-2-150x150.png 150w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/moire_graphene_on_bn_small-2-768x768.png 768w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/moire_graphene_on_bn_small-2.png 1034w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n\n\n\n<figure class=\"wp-block-image size-large\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"1024\" data-id=\"396\" src=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/moire-on-slide_-BLG-on-BN-1-1024x1024.png\" alt=\"\" class=\"wp-image-396\" srcset=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/moire-on-slide_-BLG-on-BN-1-1024x1024.png 1024w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/moire-on-slide_-BLG-on-BN-1-300x300.png 300w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/moire-on-slide_-BLG-on-BN-1-150x150.png 150w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/moire-on-slide_-BLG-on-BN-1-768x768.png 768w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/moire-on-slide_-BLG-on-BN-1-1536x1536.png 1536w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/07\/moire-on-slide_-BLG-on-BN-1-2048x2048.png 2048w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><\/figure>\n<figcaption class=\"blocks-gallery-caption wp-element-caption\"><strong><mark style=\"background-color:rgba(0, 0, 0, 0)\" class=\"has-inline-color has-black-color\">(Left) Moir\u00e9 superlattice formed in an aligned graphene\/BN structure on a SiO2 substrate. (Right) Moir\u00e9 pattern formed in an aligned bilayer graphene\/BN structure on a transfer slide. <\/mark><\/strong><\/figcaption><\/figure>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-full is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"1024\" height=\"1024\" src=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/09\/image.png\" alt=\"\" class=\"wp-image-455\" style=\"width:418px;height:auto\" srcset=\"https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/09\/image.png 1024w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/09\/image-300x300.png 300w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/09\/image-150x150.png 150w, https:\/\/newflats.c2n.universite-paris-saclay.fr\/wp-content\/uploads\/2024\/09\/image-768x768.png 768w\" sizes=\"auto, (max-width: 1024px) 100vw, 1024px\" \/><figcaption class=\"wp-element-caption\">Twisted bilayer graphene moire superlattice measured by LFM on a transfer slide before completing the stack.<\/figcaption><\/figure><\/div><\/div>\n<\/div>\n\n\n\n<div class=\"taggbox\"  style=\"width:100%;height:100%\" data-widget-id=\"163148\" data-tags=\"false\" ><\/div><script src=\"https:\/\/widget.taggbox.com\/embed-lite.min.js\" type=\"text\/javascript\"><\/script>\n","protected":false},"excerpt":{"rendered":"<p>Our experts: Jaime Diez Merida (LMU), Dmitri Efetov (LMU), Maelle Kapfer (UPSaclay), Gaia Maffione (UPSaclay) and Rebeca Ribeiro-Palau (CNRS) Clean exfoliated 2D materials are the<\/p>\n","protected":false},"author":3,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"footnotes":""},"class_list":["post-117","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/newflats.c2n.universite-paris-saclay.fr\/index.php?rest_route=\/wp\/v2\/pages\/117","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/newflats.c2n.universite-paris-saclay.fr\/index.php?rest_route=\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/newflats.c2n.universite-paris-saclay.fr\/index.php?rest_route=\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/newflats.c2n.universite-paris-saclay.fr\/index.php?rest_route=\/wp\/v2\/users\/3"}],"replies":[{"embeddable":true,"href":"https:\/\/newflats.c2n.universite-paris-saclay.fr\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=117"}],"version-history":[{"count":62,"href":"https:\/\/newflats.c2n.universite-paris-saclay.fr\/index.php?rest_route=\/wp\/v2\/pages\/117\/revisions"}],"predecessor-version":[{"id":480,"href":"https:\/\/newflats.c2n.universite-paris-saclay.fr\/index.php?rest_route=\/wp\/v2\/pages\/117\/revisions\/480"}],"wp:attachment":[{"href":"https:\/\/newflats.c2n.universite-paris-saclay.fr\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=117"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}