<?xml version="1.0" encoding="utf-8" standalone="yes"?><rss version="2.0" xmlns:atom="http://www.w3.org/2005/Atom" xmlns:content="http://purl.org/rss/1.0/modules/content/"><channel><title>Ultrafast-Demagnetization on David A. Reiss</title><link>https://d-a-reiss.github.io/tags/ultrafast-demagnetization/</link><description>Recent content in Ultrafast-Demagnetization on David A. Reiss</description><generator>Hugo -- 0.165.0</generator><language>en-us</language><lastBuildDate>Thu, 03 Jun 2021 00:00:00 +0000</lastBuildDate><atom:link href="https://d-a-reiss.github.io/tags/ultrafast-demagnetization/index.xml" rel="self" type="application/rss+xml"/><item><title>Ultrafast demagnetization of iron induced by optical versus terahertz pulses</title><link>https://d-a-reiss.github.io/publications/2021-chekhov-ultrafast-demagnetization-iron/</link><pubDate>Thu, 03 Jun 2021 00:00:00 +0000</pubDate><guid>https://d-a-reiss.github.io/publications/2021-chekhov-ultrafast-demagnetization-iron/</guid><description>We study ultrafast magnetization quenching of ferromagnetic iron following excitation by an optical vs a terahertz pump pulse. While the optical pump (photon energy of 3.1 eV) induces a strongly nonthermal electron distribution, terahertz excitation (~4 meV) results in a quasi-thermal perturbation of the electron population. The pump-induced spin and electron dynamics are interrogated by the magneto-optic Kerr effect (MOKE). A deconvolution procedure allows us to push the time resolution down to 130 fs, even though the driving terahertz pulse is more than 0.5 ps long. Remarkably, the MOKE signals exhibit an almost identical time evolution for both optical and terahertz pump pulses, despite the three orders of magnitude different number of excited electrons. We are able to quantitatively explain our results using a model based on quasi-elastic spin-flip scattering. It shows that in the small-perturbation limit, the rate of demagnetization of a metallic ferromagnet is proportional to the excess energy of the electrons, independent of the precise shape of their distribution. Our results reveal that the dynamics of ultrafast demagnetization and of the closely related terahertz spin transport do not depend on the pump photon energy.</description></item><item><title>Laser-induced terahertz spin transport in magnetic nanostructures arises from the same force as ultrafast demagnetization</title><link>https://d-a-reiss.github.io/publications/2022-rouzegar-thz-spin-transport/</link><pubDate>Mon, 22 Mar 2021 00:00:00 +0000</pubDate><guid>https://d-a-reiss.github.io/publications/2022-rouzegar-thz-spin-transport/</guid><description>Laser-induced terahertz spin transport (TST) and ultrafast demagnetization (UDM) are central but so far disconnected phenomena in femtomagnetism and terahertz spintronics. Here, we use broadband terahertz emission spectroscopy to reliably measure both processes in one setup. We find that the rate of UDM of a single ferromagnetic metal film F has the same time evolution as the flux of TST from F into an adjacent normal-metal layer N. This remarkable agreement shows that UDM and TST are driven by the same force, which is fully determined by the state of the ferromagnet. An analytical model consistently and quantitatively explains our observations. It reveals that both UDM in F and TST in the F|N stack arise from a generalized spin voltage, which is defined for arbitrary, nonthermal electron distributions. We also conclude that contributions due to a possible temperature difference between F and N are minor and that the spin-current amplitude can, in principle, be increased by one order of magnitude. In general, our findings allow one to apply the vast knowledge of UDM to TST, thereby opening up new pathways toward large-amplitude terahertz spin currents and, thus, energy-efficient ultrafast spintronic devices.</description></item></channel></rss>