Van der Waals heterostructure under rotation at 40 mK
Understanding the mechanism of high temperature (high Tc) superconductivity is a central problem in condensed matter physics. Van der Waals heterostructures provide novel materials as model systems for quantum phenomena. An international collaboration (Berkeley, Stanford, Shanghai, Tsukuba, Seoul) reports signatures of tunable superconductivity in these special heterostructures, detected via a sharp drop in the resistivity and a plateau in the I-V curve below 1 K.
The transport measurements are performed in a dilution cryostat with a base temperature of 40 mK achieved through careful filtering. For in-plane measurements, the atto3DR double sample rotator was used, which conveniently allows for using the full field of a single solenoid in an arbitrary orientation. The authors find transitions from the candidate superconductor to Mott insulator and metallic phases, proving that the TLG/hBN superlattice provides a unique model system to study the triangular Hubbard model and its relation to unconventional superconductivity as well as potentially novel electronic states.
Guorui Chen, et al.; arxiv:1901.04621 (2019)
Magnetoresistance of self-assembled GaMnAs based nanowires using the atto3DR
The relatively new class of self-assembled ferromagnetic nanowires could potentially be used for producing e.g. one-dimensional spin valve transistors or ferromagnetic single electron transistors, while maintaining a high flexibility in the choice of material as well as the axial and radial degrees of freedom. Due to the arbitrary orientation inherent to self-assembled materials on the substrate, typical characterization techniques such as magnetoresistance measurements conducted at cryogenic temperatures greatly benefit from the possibility to freely change the mutual orientation of external magnetic field and sample. To avoide an expensive 3D vector magnet the atto3DR, a 3-dimensional rotator offers a good a reliable solution for transport measurements which is in particular interesting in the field of mesoscopic physics at cryogenics.
Angle Dependent Magnetoresistance Measurement at Cryogenics
Due to the arbitrary orientation inherent to self-assembled materials on the substrate, typical characterization techniques such as magnetoresistance measurements conducted at cryogenic temperatures greatly benefit from the possibility to freely change the mutual orientation of external magnetic field and sample. Although this is easily possible e.g. by using a 3D vector magnet setup, the associated costs (>> 100 k$) are often prohibitive. Single axis sample rotator setups on the other hand not only require choosing either an out-of-plane or in-plane configuration prior to cooldown, but also put firm restrictions on certain measurements which rely on a precise orientation of the field e.g. perpendicular or parallel to an initially unknown direction along a sample structure. The perfect solution to such applications is attocube’s 3-dimensional rotator atto3DR.
Similar to a recent publication by C. H. Butschkow and co-workers from the group of Prof. Dieter Weiss (Univ. of Regensburg), magnetotransport measurements on individual GaAs/(Ga,Mn)As core-shell nanowires (top figure) have been conducted.
The center figure shows magnetoresistance at 5 T as a function of the angle between externally applied magnetic field and the nanowire axis for different rotation planes: (orange) in-plane rotation, referring to the SiO2 substrate plane, (green) out of plane (perpendicular) rotation with the long nanowire axis (typically 4 µm long and 100 nm in diameter) entirely in the rotation plane, and (blue) out of plane (transversal) rotation with the rotation plane transversal to the nanowire axis.
The bottom figure shows the normalized magnetoresistance as a function of the angle between externally applied magnetic field and the nanowire axis for various magnitudes of the external magnetic field.
(measured by C. Butschkow in collaboration with attocube application labs 2012; sample courtesy of C. Butschkow, University of Regensburg).
This measurement was realized with the atto3DR.
C. Butschkow et al., Phys. Rev. B 87, 245303 (2013)