SPASER As a Complex System: Femtosecond Dynamics Traced by Ab-Initio Simulations
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Phase Transitions in Spin Glasses
Phase Transitions in Spin Glasses Peter Young Talk available at http://physics.ucsc.edu/˜peter/talks/columbia.pdf e-mail:[email protected] Supported by the Hierarchical Systems Research Foundation. Recent collaborators: H. G. Katzgraber, L. W. Lee, J. Pixley, D. Larson, V. Martin-Mayor, A. Tarancon, L. A. Fernandez, S. Gaviro, Colloquium at Columbia University, October 19, 2009. – p.1 Overview • Basic Introduction • What is a spin glass? Why are they important? • Why are Monte Carlo simulations for spin glasses hard? • Try to answer two important questions concerning phase transitions in spin glasses: • Is there a phase transition in an isotropic Heisenberg spin glass? • Is there a transition in an Ising spin glass in a magnetic field (Almeida-Thouless line)? – p.2 What is a spin glass? A system with disorder and frustration. or Most theory uses the simplest model with these ingredients: the Edwards-Anderson Model: H = − Jij Si · Sj − hi · Si . i,j i hXi X Interactions are quenched and are random (have either sign). 2 1/2 Take a Gaussian distribution: [Jij ]av = 0; [Jij ]av = J (= 1) Spins, Si, fluctuate and have m–components: m = 1 (Ising) m = 2 (XY) m = 3 (Heisenberg). – p.3 Spin Glass Systems • Metals: Diluted magnetic atoms, e.g. Mn, in non-magnetic metal, e.g. Cu. RKKY interaction: cos(2kF Rij ) Jij ∼ 3 Rij Random in magnitude and sign, which gives frustration. Note: Mn (S-state ion) has little anisotropy; → Heisenberg spin glass. • Important because relevant to other systems: • “Vortex glass” transition in superconductors • Optimization problems in computer science (including solving optimization problems on a quantum computer) • Protein folding • Error correcting codes – p.4 Slow Dynamics (free) energy Slow dynamics The dynamics is very slow barrier at low T . -
Arxiv:Cond-Mat/0503344 V1 15 Mar 2005 Local Vs. Global Variables For
Local vs. Global Variables for Spin Glasses C. M. Newman∗ D. L. Stein† newman@ cims.nyu.edu dls @ physics.arizona.edu Courant Institute of Mathematical Sciences Depts. of Physics and Mathematics New York University University of Arizona New York, NY 10012, USA Tucson, AZ 85721, USA Abstract We discuss a framework for understanding why spin glasses differ so remarkably from ho- mogeneous systems like ferromagnets, in the context of the sharply divergent low temperature behavior of short- and infinite-range versions of the same model. Our analysis is grounded in understanding the distinction between two broad classes of thermodynamic variables – those that describe the global features of a macroscopic system, and those that describe, or are sen- sitive to, its local features. In homogeneous systems both variables generally behave similarly, but this is not at all so in spin glasses. In much of the literature these two different classes of variables were commingled and confused. By analyzing their quite different behaviors in finite- and infinite-range spin glass models, we see the fundamental reason why the two sys- tems possess very different types of low-temperature phases. In so doing, we also reconcile apparent discrepancies between the infinite-volume limit and the behavior of large, finite vol- umes, and provide tools for understanding inhomogeneous systems in a wide array of contexts. We further propose a set of ‘global variables’ that are definable and sensible for both short- range and infinite-range spin glasses, and allow a meaningful basis for comparison of their arXiv:cond-mat/0503344 v1 15 Mar 2005 low-temperature properties. -
Study of Spin Glass and Cluster Ferromagnetism in Rusr2eu1.4Ce0.6Cu2o10-Δ Magneto Superconductor Anuj Kumar, R
Study of spin glass and cluster ferromagnetism in RuSr2Eu1.4Ce0.6Cu2O10-δ magneto superconductor Anuj Kumar, R. P. Tandon, and V. P. S. Awana Citation: J. Appl. Phys. 110, 043926 (2011); doi: 10.1063/1.3626824 View online: http://dx.doi.org/10.1063/1.3626824 View Table of Contents: http://jap.aip.org/resource/1/JAPIAU/v110/i4 Published by the American Institute of Physics. Related Articles Annealing effect on the excess conductivity of Cu0.5Tl0.25M0.25Ba2Ca2Cu3O10−δ (M=K, Na, Li, Tl) superconductors J. Appl. Phys. 111, 053914 (2012) Effect of columnar grain boundaries on flux pinning in MgB2 films J. Appl. Phys. 111, 053906 (2012) The scaling analysis on effective activation energy in HgBa2Ca2Cu3O8+δ J. Appl. Phys. 111, 07D709 (2012) Magnetism and superconductivity in the Heusler alloy Pd2YbPb J. Appl. Phys. 111, 07E111 (2012) Micromagnetic analysis of the magnetization dynamics driven by the Oersted field in permalloy nanorings J. Appl. Phys. 111, 07D103 (2012) Additional information on J. Appl. Phys. Journal Homepage: http://jap.aip.org/ Journal Information: http://jap.aip.org/about/about_the_journal Top downloads: http://jap.aip.org/features/most_downloaded Information for Authors: http://jap.aip.org/authors Downloaded 12 Mar 2012 to 14.139.60.97. Redistribution subject to AIP license or copyright; see http://jap.aip.org/about/rights_and_permissions JOURNAL OF APPLIED PHYSICS 110, 043926 (2011) Study of spin glass and cluster ferromagnetism in RuSr2Eu1.4Ce0.6Cu2O10-d magneto superconductor Anuj Kumar,1,2 R. P. Tandon,2 and V. P. S. Awana1,a) 1Quantum Phenomena and Application Division, National Physical Laboratory (CSIR), Dr. -
Arxiv:1902.01645V1 [Cond-Mat.Mtrl-Sci] 5 Feb 2019 Magnetic Phases of Fe-Cr Alloys Are Fairly Complex
The Dynamics of Magnetism in Fe-Cr Alloys with Cr Clustering Jacob B. J. Chapman,∗ Pui-Wai Ma, and S. L. Dudarev UK Atomic Energy Authority, Culham Science Centre, Oxfordshire, OX14 3DB, United Kingdom The dynamics of magnetic moments in iron-chromium alloys with different levels of Cr clustering show unusual features resulting from the fact that even in a perfect body-centred cubic structure, magnetic moments experience geometric magnetic frustration resembling that of a spin glass. Due to the long range exchange coupling and configuration randomness, magnetic moments of Cr solutes remain non-collinear at all temperatures. To characterise magnetic properties of Fe-Cr alloys, we explore the temperature dependence of magnetisation, susceptibility, Curie temperature and spin- spin correlations with spatial resolution. The static and dynamic magnetic properties are correlated with the microstructure of Fe-Cr, where magnetisation and susceptibility are determined by the size of Cr precipitates at nominal Cr concentrations. The Curie temperature is always maximised when the solute concentration of Cr in the α phase is close to 5 to 6 at.%, and the susceptibility of Fe atoms is always enhanced at the boundary between a precipitate and solid solution. Interaction between Cr and Fe stimulates magnetic disorder, lowering the effective Curie temperature. Dynamic simulation of evolution of magnetic correlations shows that the spin-spin relaxation time in Fe-Cr alloys is in the 20 to 40 ps range. I. INTRODUCTION and 84 at.% Cr, Fe magnetic moments prevent long range AFM-like correlations, causing the moments to freeze 15 Iron and chromium are the main components of steels. -
Bose-Einstein Condensation in Quantum Glasses
Motivations The quantum cavity method A lattice model for the superglass Discussion Conclusions Bose-Einstein condensation in Quantum Glasses Giuseppe Carleo, Marco Tarzia, and Francesco Zamponi∗ Phys. Rev. Lett. 103, 215302 (2009) Collaborators: Florent Krzakala, Laura Foini, Alberto Rosso, Guilhem Semerjian ∗Laboratoire de Physique Th´eorique, Ecole Normale Sup´erieure, 24 Rue Lhomond, 75231 Paris Cedex 05 March 29, 2010 Motivations The quantum cavity method A lattice model for the superglass Discussion Conclusions Outline 1 Motivations Supersolidity of He4 Helium 4: Monte Carlo results 2 The quantum cavity method Regular lattices, Bethe lattices and random graphs Recursion relations Bose-Hubbard models on the Bethe lattice 3 A lattice model for the superglass Extended Hubbard model on a random graph Results A variational argument 4 Discussion Disordered Bose-Hubbard model: the Bose glass 3D spin glass model with quenched disorder Quantum Biroli-M´ezard model: a lattice glass model 5 Conclusions Motivations The quantum cavity method A lattice model for the superglass Discussion Conclusions Outline 1 Motivations Supersolidity of He4 Helium 4: Monte Carlo results 2 The quantum cavity method Regular lattices, Bethe lattices and random graphs Recursion relations Bose-Hubbard models on the Bethe lattice 3 A lattice model for the superglass Extended Hubbard model on a random graph Results A variational argument 4 Discussion Disordered Bose-Hubbard model: the Bose glass 3D spin glass model with quenched disorder Quantum Biroli-M´ezard model: a lattice glass model 5 Conclusions Experimental Results Discovery by Kim & Chan in He4 (Nature & Science 2004). Motivations• The quantumExperimental cavity method A lattice modelResults for the superglass Discussion Conclusions Reproduced after by many4 other groups. -
Introduction to AC Susceptibility
QuantumDesign Introduction to: AC Susceptibility AC Magnetic Measurements Dinesh Martien Introduction AC magnetic measurements, in which an AC field is applied to a sample and the resulting AC moment is measured, are an important tool for characterizing many materials. Because the induced sample moment is time-dependent, AC measurements yield information about magnetization dynamics which are not AC Magnetometry obtained in DC measurements, where the sample moment is constant during the measurement time. This application note In AC magnetic measurements, a small AC drive magnetic field will briefly describe how AC magnetic measurements are is superimposed on the DC field, causing a time-dependent performed, discuss the meaning of the data that come out of moment in the sample. The field of the time-dependent an AC measurement, and show some measurement examples. moment induces a current in the pickup coils, allowing meas- urement without sample motion. The detection circuitry is configured to detect only in a narrow frequency band, normally DC Magnetometry at the fundamental frequency (that of the AC drive field). DC magnetic measurements determine the equilibrium value In order to understand what is measured in AC magnetometry, of the magnetization in a sample. The sample is magnetized first consider very low frequencies, where the measurement is by a constant magnetic field and the magnetic moment of the most similar to DC magnetometry. In this case, the magnetic sample is measured, producing a DC magnetization curve moment of the sample follows the M(H) curve that would be M(H) . The moment is measured by force, torque or induc- measured in a DC experiment. -
Synthesis and SERS Application of Sio2@Au Nanoparticles
Synthesis and SERS application of SiO2@Au nanoparticles A. Saini, T. Maurer*, I. Izquierdo Lorenzo, A. Ribeiro Santos, J. Béal, J. Goffard, D. Gérard, A. Vial and J. Plain Laboratoire de Nanotechnologie et d’Instrumentation Optique, ICD CNRS UMR n°6281, Université de Technologie de Troyes, CS 42060, 10004 Troyes, France In this letter, we report a chemical route for synthesizing SiO2@Au core-shell nanoparticles. The process includes four steps: i) preparation of the silica cores, ii) grafting gold nanoparticles over SiO2 cores, iii) priming of the silica-coated gold nanoparticles with 2 and 10 nm gold colloids and finally iv) formation of complete shell. The optical extinction spectra were experimentally measured and compared to numerical calculations in order to confirm the dimensions deduced from SEM images. Finally, the potential of such core- shell nanoparticles for biosensing was probed by means of Surface Enhanced Raman Scattering measurements and revealed higher sensitivities with much lower gold quantity of such core-shell nanoparticles compared to Au nanoparticles exhibiting similar diameters. SiO2 core-Au shell nanoparticles have attracted much attention for the past ten years due to potential applications in various fields such as cancer imaging and treatment(Loo et al., 2004), Surface-Enhanced Raman Spectroscopy (SERS) detection of molecules(Wang et al., 2006, Maurer et al., 2013), catalytic degradation of environmental pollutants(Ma et al., 2009) or even fabrication of SPASER (Surface Plasmon Amplification by Stimulated Emission of radiation) devices when the silica is dye-doped(Stockman, 2008). However, the growth of a complete gold shell around silica nanoparticles is very hard to achieve. -
Aging, Rejuvenation and Memory : the Example of Spin Glasses
Aging, rejuvenation and memory : the example of spin glasses Eric VINCENT Service de Physique de l’Etat Condensé (CNRS URA 2464), DSM/DRECAM/SPEC, CEA Saclay, 91191 Gif sur Yvette Cedex, France [email protected] This paper is written on the basis of a course given at the summer school “Ageing and the glass transition” in the University of Luxembourg. The results presented here are the joint work of the Saclay group: F. Bert, J.-P. Bouchaud, V. Dupuis, J. Hammann, D. Hérisson, F. Ladieu, M. Ocio, D. Parker, E.V., and others. 1. What is a spin glass ? 2. Slow dynamics and aging 2.1 DC experiments 2.2 AC susceptibility 2.3 Noise measurements 2.4 Rejuvenation by a stress 3. Aging, rejuvenation and memory 3.1 Cooling rate effects 3.2 Memory dip experiments 3.3 Rejuvenation and memory versus cumulative aging 4. Characteristic length scales for aging 4.1 Length scales from field variation experiments 4.2 Length scales from temperature variation experiments 4.3 The dynamical correlation length from both temperature and field variation experiments 4.4 Separation of time and length scales with temperature: how much ? 5. Conclusions Abstract - In this paper, we review the general features of the out-of-equilibrium dynamics of spin glasses. We use this example as a guideline for a brief description of glassy dynamics in other disordered systems like structural and polymer glasses, colloids, gels etc. Starting with the simplest experiments, we discuss the scaling laws used to describe the isothermal aging observed in spin glasses after a quench down to the low temperature phase (these scaling laws are the same as established for polymer glasses). -
The Physics of the Colloidal Glass Transition
Home Search Collections Journals About Contact us My IOPscience The physics of the colloidal glass transition This article has been downloaded from IOPscience. Please scroll down to see the full text article. 2012 Rep. Prog. Phys. 75 066501 (http://iopscience.iop.org/0034-4885/75/6/066501) View the table of contents for this issue, or go to the journal homepage for more Download details: IP Address: 190.55.69.57 The article was downloaded on 17/05/2012 at 00:32 Please note that terms and conditions apply. IOP PUBLISHING REPORTS ON PROGRESS IN PHYSICS Rep. Prog. Phys. 75 (2012) 066501 (30pp) doi:10.1088/0034-4885/75/6/066501 The physics of the colloidal glass transition Gary L Hunter and Eric R Weeks Department of Physics, Emory University, Math and Science Center 400 Dowman Dr., N201 Atlanta, GA 30322, USA E-mail: [email protected] Received 26 June 2011, in final form 15 March 2012 Published 16 May 2012 Online at stacks.iop.org/RoPP/75/066501 Abstract As one increases the concentration of a colloidal suspension, the system exhibits a dramatic increase in viscosity. Beyond a certain concentration, the system is said to be a colloidal glass; structurally, the system resembles a liquid, yet motions within the suspension are slow enough that it can be considered essentially frozen. For several decades, colloids have served as a valuable model system for understanding the glass transition in molecular systems. The spatial and temporal scales involved allow these systems to be studied by a wide variety of experimental techniques. -
Emergence of Griffiths Phase, Re-Entrant Cluster Glass,Metamagnetic Transition
Emergence of Griffiths phase, re-entrant cluster glass,metamagnetic transition and field induced unusual spin dynamics in Tb2CoMnO6 Khyati Anand1, Arkadeb Pal1, Prajyoti Singh1, Md. Alam1, Amish G Joshi2, Anita Mohan1 and Sandip Chatterjee1,# 1Indian Institute of Technology (BHU) Varanasi 221005, India 2CSIR- Central Glass & Ceramic Research Institute, Ahmadabad 382330, India #Corresponding Email: [email protected] Abstract The structural and magnetic properties of double perovskiteTb2CoMnO6 have been investigated. Electronic structure analysis by XPS study reveals the presence of mixed oxidation state (Mn4+/Mn3+ and Co2+/Co3+) of B-site ions. The dc and ac magnetization measurements reveal different interesting phases such as Griffith phase, re-entrant spin glass, metamagnetic steps, Hopkinson like peak and also unusual slow relaxation. The M-H curve indicates the presence of competing AFM/FM interactions. The disorder in Tb2CoMnO6 leads to spin frustration at low temperature givingrise to the re-entrant spin glass. Moreover, the field-dependent ac susceptibility studiesunraveled the presence of Hopkinson like peak associated with the domain wall motion and the large anisotropy field.The further study yielded that the relaxation associated with this peak is unusually slow. Introduction The materials that possess both the magnetic and electric orders have received intense research attention globally owing to their potential for practical applications in next generation spintronic devices [1–5]. The coupling among the different order parameters allows one to have freedom of an additional gauge for monitoring one of these order parameters by the other which opens up unprecedented opportunities to achieve new functionalities in such materials [1–8]. Hence, an invigorated research attention has been bestowed on discovering such multifunctional materials and there is also an on-going search for the new mechanisms leading to such coupled order parameters. -
Experiment and Theory: No Spasing from Core-Shell Spasers
Experiment and Theory: No Spasing from Core-Shell Spasers Günter Kewes,1 Kathrin Höfner,2 Andreas Ott,3 Rogelio Rodriguez-Oliveros,2 Alexander Kuhlicke,1 Yan Lu,3 Matthias Ballauff,3 Kurt Busch,2, 4 and Oliver Benson1 1AG Nanooptik, Institut für Physik, Humboldt-Universität zu Berlin, Newtonstrasse 15, 12489 Berlin, Germany 2AG Theoretische Optik & Photonik, Institut für Physik, Humboldt-Universität zu Berlin, Newtonstrasse 15, 12489 Berlin, Germany 3Helmholtz-Zentrum Berlin für Materialien und Energie GmbH (HZB), Hahn-Meitner-Platz 1, 14109 Berlin, Germany 4Max-Born Institut, Max-Born-Strasse 2a, 12489 Berlin, Germany In 2009 the smallest laser-device consisting of a single 14 nm gold sphere and a dye-doped coating was “demonstrated” [1] based on the proposal of the “spaser” from 2003 [2]. Here, we critically evaluate so far reported results on both an experimental and on a theoretical basis. Experiments: Core-shell spasers were chemically synthesized or metal nanoparticles were coated with dye-doped polymer films. Various excitation schemes were tested, yielding laser or laser-like signatures. All of them, however, were later identified to stem from sources other than spasing. Theory: A fully analytic model for spherical core-shell spasers was developed: Within this model, we drop the widely used quasi-static approximation of the electromagnetic field in favor of fully electromagnetic Mie theory. This allows for precise incorporation of realistic gain relaxation rates (quenching and cavity-to-gain coupling) that so far have only been estimated (and massively underestimated) in spaser theory. The model unravels multiple severe limitations (that exist all over the VIS) concerning the threshold-pump, the extreme gain-medium requirements and the unavoidable heat production (independent of excitation scheme). -
Plasmon Lasers
Plasmon Lasers Wenqi Zhu1,2, Shawn Divitt1,2, Matthew S. Davis1, 2, 3, Cheng Zhang1,2, Ting Xu4,5, Henri J. Lezec1 and Amit Agrawal1, 2* 1Center for Nanoscale Science and Technology, National Institute of Standards and Technology, Gaithersburg, MD 20899 USA 2Maryland NanoCenter, University of Maryland, College Park, MD 20742 USA 3Department of Electrical Engineering and Computer Science, Syracuse University, Syracuse, NY 13244 USA 4National Laboratory of Solid-State Microstructures, Jiangsu Key Laboratory of Artificial Functional Materials, College of Engineering and Applied Sciences, Nanjing University, Nanjing, China 5Collaborative Innovation Center of Advanced Microstructures, Nanjing, China Corresponding*: [email protected] Recent advancements in the ability to design, fabricate and characterize optical and optoelectronic devices at the nanometer scale have led to tremendous developments in the miniaturization of optical systems and circuits. Development of wavelength-scale optical elements that are able to efficiently generate, manipulate and detect light, along with their subsequent integration on functional devices and systems, have been one of the main focuses of ongoing research in nanophotonics. To achieve coherent light generation at the nanoscale, much of the research over the last few decades has focused on achieving lasing using high- index dielectric resonators in the form of photonic crystals or whispering gallery mode resonators. More recently, nano-lasers based on metallic resonators that sustain surface plasmons – collective electron oscillations at the interface between a metal and a dielectric – have emerged as a promising candidate. This article discusses the fundamentals of surface plasmons and the various embodiments of plasmonic resonators that serve as the building block for plasmon lasers.