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If the solution you need is not on the list, please go ahead and order this product. During the check out please identify the material you need along with any specifications you have in mind. Our R&D team will promptly get back to you and start to...

As2Te3 single crystals are crystallized in the α phase and belongs to monoclinic C2/m space group. As2Te3 crystals exhibit topological insulator and thermoelectric behavior, in the bulk it is a narrow gap semiconductor with ~0.24 eV band gap...

The only commercially available topological insulator thalium alloyed BiTlTe (bismuth thallium telluride) crystals. Tl has been alloyed into Bi2Te3 matrix to create Bi(2-x)TlxTe3 crystals at x=0.7 and x=1.3 ranges. BiTlTe (thalium doped Bi2Te3 crystals)...

Bi2SeTe2 is a topological insulator vdW layered crystal. It has the same crystal structure as Bi2Se3 and Bi2Te3, it only differs in that Se and Te atoms are alloyed to retain impressive topological insulator state rivaling to Bi2Te3. Bi2SeTe3 crystal...

BiInTe3 layered crystals crystallize in M2X3 structure where M stands for Bi and In atoms at fixed 50% alloy ratios. BiInTe3 crystals were synthesized using modified Bridgman technique under careful growth condition to ensure there is no phase separation...

BiSbTe3 is a layered topological insulator material belonging to Bi2Te3 and Sb2Te3 proto-type material systems. Each layer consists of BiSbTe3 sheets weakly interacting through van der Waals (vdW) interactions. Explicit chemical formula can be written as...

Bi1.5Sb0.5Te1.7Se1.3 or in shortly BSTS is a vdW topological material and vdW superconductor with exciting superconducting properties from bulk to monolayer scales. BSTS is a 3D topological insulator and superconductor and the...

Bismuth telluride (BiTe) is an intermediate composition material in Bismuth chalcogen material family. It exhibits rather unusual material properties including topological response, low temperature superconductivity, semimatellicity, as well as CDWs...

CdI₂ is a layered semiconductor with indirect gap at 3.0 eV for bulk and its properties in the monolayer form is currently unknown. It crystallizes in generally known as CdI2 crystal structure as shown in the product images. The repeating...

Cr2S3 is ferrimagnetic layered semiconductor in its bulk form with Tc≈125 K. Cr2S3 crystallizes in rhombohedral R¯3 geometry and exhibit rather unique structure. Our Cr2S3 crystals are highly layered and very easy to exfoliate with similar...

The only magnetic grade CrCl3 vdW crystals in the commercial market. Our customers knows that slim amount of defects and magnetic impurities are sufficient to mask the observation of exotic magnetic behavior from 2D magnets. Our vdW magnets are created...

CrI3 vdw crystals were synthesized through high-quality self-flux technique without using any contaminating transport agents. Our CrI3 crystals come with guaranteed magnetic response and typical crystals measure around 0.5cm in size. Samples are packaged...