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INSULATOR METAL TRANSITION AT THE NANOSCALE

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An international team of researchers has been able to probe the insulator-conductor phase transition of materials at the nanoscale resolution. This is one of the first results of MaReS endstation of BOREAS beamline.

Cerdanyola del Vallès, 8 June 2018. Controlling the flow of electrons within circuits is how electronic devices work. This is achieved through the appropriate choice of materials. Metals allow electrons to flow freely and insulators prevent conduction. In general, the electrical properties of a material are determined when the material is fabricated and cannot be changed afterwards without changing the material. However, there are materials that can exhibit metal or insulator behaviour depending on their temperature. Being able switch their properties, these materials could lead to a new generation of electronic devices.

Vanadium Dioxide (VO2) is one such material. It can switch from an insulating phase to a metallic phase just above room temperature, a feature exploited already for sensors. However, the reason why the properties of this material change so dramatically has been a matter of scientific debate for over 50 years.

One of the challenges in understanding why and how this switch occurs is due to a process called phase separation. The insulator-metal phase transition is similar to the ice to liquid transition in water. When ice melts, both liquid and solid water can coexist in separate regions. Similarly, in VO2, insulating and metallic regions of the material can be coexisting at the same time during the transition. But unlike water, where the different regions are often large enough to see with the naked eye, in VOthis separation occurs on the nanoscale and it is thus challenging to observe. As a result, it has been hard to know if the true properties of each phase, or the mixture of both phases, are being measured.

X-rays are a key tool for understanding the properties of materials, but it has been hard to use them to probe materials on the nanoscale because it is hard to build lenses for microscopes that can detect them. However, in this study published in Nano Letters, a team of researchers from Institute of Photonic Sciences (ICFO) and ALBA in Barcelona, the Technisch Universitat and Max-Born Institute in Berlin, and Vanderbilt Universityin Tennessee, has finally been able to probe the phase transitions that occur in thin films of Vanadium Dioxide (VO2) using resonant soft X-ray holography. This technique, based on the interference of the beam transmitted through the sample and a reference aperture, enables imaging the electronic and structural changes in this material with an unprecedented resolution at the nanoscale without the need of a lens. By looking at the material with 50 nm resolution, the scientists were able to observe that defects in the material played an important role in initiating the phase transition from the insulator to the metal. However, more importantly, the authors also observed a third intermediate state formed during the phase transformation. Whilst some regions transformed directly from the insulating to metallic phase, others transformed into a second different insulating state before becoming metallic at higher temperatures with the exact pathway taken depending on the defects present in the material. The coexistences of three phases has radically changed the views of previous studies that assumed the presence of only two states during the transition. Even more, the study presents new ways in which the transition could be controlled.

In addition to the results obtained on the phase transition in VO2, the work also highlights the possibilities that X-ray holography can bring for studying materials on the nanoscale. The technique is a unique method to image real-time nanoscale dynamics and is now being used to study the properties of other intriguing materials such as high temperature superconductors. Such a technique is becoming a relevant cutting edge approach implemented at a few synchrotrons in the world, and these results demonstrate is available at the multipurpose resonant scattering endstation, MaReS, of BOREAS beamline in ALBA.

IM_BOREAS_SoftXRayHolography 

Figure1: Illustration of the concept for Soft x-ray holography, together with x-ray holograms and Fourier transformed reconstructed holograms with nanoscale resolution and demonstration of the exploited x-ray linear dichroism mechanism as imaging contrast.

IM_BOREAS_PhaseTransitionVO2

Figure 2: (left) Phase transition from insulator to metallic phase in VO2 as a function of the temperature, with contrast exploiting linear x-ray dichroism; (right) reconstructed holograms at the vanadium and oxygen edges (518, 529, and 530.5 eV) used to encode the intensities of the three color channels of an RGB (red, green, blue) image. At 330 K, an increase in intensity of the green channel, which probes the metallic rutile phase (R) through the d∥ state, is observed in small regions. As the sample is heated further, it becomes increasingly clear that the blue channel, which probes a intermediate insulating M2 phase, also changes but in different regions. At 334 K, three distinct regions can be observed corresponding to the insulating monoclinic M1, M2, and metallic R phases. As the temperature increases, the R phase dominates. The circular field of view is 2 μm in diameter. (taken from Vidas et al, Nanoletters, 2018).

Reference: Imaging Nanometer Phase Coexistence at Defects During the Insulator–Metal Phase Transformation in VO2 Thin Films by Resonant Soft X-ray Holography Nanoletters (2018) DOI: 10.1021/acs.nanolett.8b00458

Acknowledgements: L.V. and T.A.M. thankfully acknowledge financial support by the HZB. S.W. acknowledges financial support from Spanish MINECO (Severo Ochoa Grant SEV-2015-0522), Ramoń y Cajal programme RYC-2013-14838, Marie Curie Career Integration Grant PCIG12-GA-2013-618487, Fundació Privada Cellex, and CERCA Programme/Generalitat de Catalunya. Research at Vanderbilt was supported by the United States National Science Foundation (EECS-1509740 for K.A.H., DMR-1207507 for R.E.M.).

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