Magnetotransport Studies of Organic Spin Valves A. M. Goldman, University of Minnesota, DMR-0414890 Graph of the resistance versus magnetic field at 100K.

Slides:



Advertisements
Similar presentations
MICROWAVE FET Microwave FET : operates in the microwave frequencies
Advertisements

by Alexander Glavtchev
CONTENTS 1. History 2. FET Definition 3. FET operation
Metal Oxide Semiconductor Field Effect Transistors
(Neil weste p: ).  A MOS transistor is a majority-carrier device, in which the current in a conducting channel between the source and the drain.
Spintronics The Search for Effective Spin Polarized Current Injection Into Semiconductors Presented by Alan Gabel Boston University Introduction to Solid.
Chapter 6 The Field Effect Transistor
Semiconductor basics 1. Vacuum tubes  Diode  Triode 2. Semiconductors  Diode  Transistors Bipolar Bipolar Field Effect Field Effect 3. What’s next?
NAME OF FACULTY : MR. Harekrushna Avaiya DEPARTMENT: E.C. (PPI-1ST) BASIC ELECTRONICS.
Field-effect transistors ( FETs) EBB424E Dr. Sabar D. Hutagalung School of Materials & Mineral Resources Engineering, Universiti Sains Malaysia.
Lecture 15 OUTLINE MOSFET structure & operation (qualitative)
MOS Capacitors ECE Some Classes of Field Effect Transistors Metal-Oxide-Semiconductor Field Effect Transistor ▫ MOSFET, which will be the type that.
Metal-Oxide-Semiconductor Field Effect Transistors
Field-Effect Transistor
Qualitative Discussion of MOS Transistors. Big Picture ES220 (Electric Circuits) – R, L, C, transformer, op-amp ES230 (Electronics I) – Diodes – BJT –
Principles & Applications
Emerging Memory Technologies
Transition Metal Doped Sb 2 Te 3 and Bi 2 Te 3 Diluted Magnetic Semiconductors Ctirad Uher DMR By low temperature MBE technique, we were able to.
G.K.BHARAD INSTITUTE OF ENGINEERING DIVISION :D (C.E.) Roll Number :67 SUBJECT :PHYSICS SUBJECT CODE : Presentation By: Kartavya Parmar.
Penn ESE370 Fall DeHon 1 ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems Day 10: September 28, 2011 MOS Transistor.
Electronic Devices Laboratory CE/EE 3110 Conductivity and the Hall Effect.
Ravi Sharma Co-Promoter Dr. Michel Houssa Electrical Spin Injection into p-type Silicon using SiO 2 - Cobalt Tunnel Devices: The Role of Schottky Barrier.
1 Conceptual Physics Study Notes & Questions: Conductors, Etc. (Chap. 24) 1)In conductors, the material’s valence electrons are free to move between neighboring.
Chapter Intrinsic: -- case for pure Si -- # electrons = # holes (n = p) Extrinsic: -- electrical behavior is determined by presence of impurities.
Penn ESE370 Fall DeHon 1 ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems Day 8: September 24, 2010 MOS Model.
Field Effect Transistor. What is FET FET is abbreviation of Field Effect Transistor. This is a transistor in which current is controlled by voltage only.
Filed Effect Transistor.  In 1945, Shockley had an idea for making a solid state device out of semiconductors.  He reasoned that a strong electrical.
NMOS PMOS. K-Map of NAND gate CMOS Realization of NAND gate.
Penn ESE370 Fall DeHon 1 ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems Day 9: September 17, 2014 MOS Model.
Short Channel Effects in MOSFET
INTEGRATED CIRCUITS Dr. Esam Yosry Lec. #3. Diffusion  Introduction  Diffusion Process  Diffusion Mechanisms  Why Diffusion?  Diffusion Technology.
Influence of carrier mobility and interface trap states on the transfer characteristics of organic thin film transistors. INFM A. Bolognesi, A. Di Carlo.
Vanderbilt MURI meeting, June 14 th &15 th 2007 Band-To-Band Tunneling (BBT) Induced Leakage Current Enhancement in Irradiated Fully Depleted SOI Devices.
ECE442: Digital ElectronicsCSUN, Spring-2010-Zahid MOS Transistor ECE442: Digital Electronics.
UNIT I MOS TRANSISTOR THEORY AND PROCESS TECHNOLOGY
VLSI System Design Lect. 2.2 CMOS Transistor Theory2 Engr. Anees ul Husnain ( Department of Electronics.
Master Colloquium Field-effect Control of Insulator-metal Transition Property in Strongly Correlated (La,Pr,Ca)MnO 3 Film Ion Liquid (IL) LPCMO channel.
Introduction to Spintronics
Penn ESE370 Fall DeHon 1 ESE370: Circuit-Level Modeling, Design, and Optimization for Digital Systems Day 9: September 26, 2011 MOS Model.
1 Other Transistor Topologies 30 March and 1 April 2015 The two gate terminals are tied together to form single gate connection; the source terminal is.
MOS Capacitors UoG-UESTC Some Classes of Field Effect Transistors Metal-Oxide-Semiconductor Field Effect Transistor ▫ MOSFET, which will be the.
Fowler-Nordheim Tunneling in TiO2 for room temperature operation of the Vertical Metal Insulator Semiconductor Tunneling Transistor (VMISTT) Lit Ho Chong,Kanad.
Source-gated Transistor Seokmin Hong. Why do we need it? * Short Channel Effects Source/Drain Charge Sharing Drain-Induced Barrier Lowering Subsurface.
Metal-oxide-semiconductor field-effect transistors (MOSFETs) allow high density and low power dissipation. To reduce system cost and increase portability,
Preliminary doping dependence studies indicate that the ISHE signal does pass through a resonance as a function of doping. The curves below are plotted.
Field Effect Transistor (FET)
Farzana R. ZakiCSE 177/ EEE 1771 Lecture – 19. Farzana R. ZakiCSE 177/ EEE 1772 MOSFET Construction & operation of Depletion type MOSFET Plotting transfer.
Carrier Motion - Electric Fields ECE Movement of Electrons and Holes Nearly free electrons can easily move in a semiconductor since they are not.
EE 466/586 VLSI Design Partha Pande School of EECS Washington State University
Deep Level Transient Spectroscopy study of 3D silicon Mahfuza Ahmed.
Fatemeh (Samira) Soltani University of Victoria June 11 th
Damu, 2008EGE535 Fall 08, Lecture 21 EGE535 Low Power VLSI Design Lecture #2 MOSFET Basics.
CMOS VLSI Design 4th Ed. EEL 6167: VLSI Design Wujie Wen, Assistant Professor Department of ECE Lecture 3A: CMOs Transistor Theory Slides adapted from.
Introduction to MOS Transistors
EE314 IBM/Motorola Power PC620 IBM Power PC 601 Motorola MC68020 Field Effect Transistors.
The Devices: MOS Transistor
Chapter 6 The Field Effect Transistor
Day 9: September 27, 2010 MOS Transistor Basics
MOS Field-Effect Transistors (MOSFETs)
Other Transistor Topologies
Recall Last Lecture Common collector Voltage gain and Current gain
Single-molecule transistors: many-body physics and possible applications Douglas Natelson, Rice University, DMR (a) Transistors are semiconductor.
Metal Semiconductor Field Effect Transistors
Day 9: September 18, 2013 MOS Model
منبع: & کتابMICROELECTRONIC CIRCUITS 5/e Sedra/Smith
Short channel effects Zewei Ding.
Other Transistor Topologies
Optically Reconfigurable Dielectrics in Ultra-Thin Transistors
Solid State Electronics ECE-1109
Other Transistor Topologies
Presentation transcript:

Magnetotransport Studies of Organic Spin Valves A. M. Goldman, University of Minnesota, DMR Graph of the resistance versus magnetic field at 100K. Gate and drain voltages were -80V and -4V, respectively. The horizontal arrows indicate the direction of the applied magnetic field. The vertical arrows indicate the relative magnetizations of the two ferromagnetic contacts. Spin transport through organic semiconductors (OSCs) is of interest because OSCs are expected to have longer spin diffusion lengths than inorganic semiconductors. Organic field effect transistors with ferromagnetic source/drain contacts are being used to observe spin tran- sport. The gate voltage induces carriers in the OSC, and by changing the relative magne- tizations of the two ferromagnetic contacts the current flow can be modulated. We have ob- served big changes of resistance when negative gate voltages are applied to induce holes and the magnetic field is swept to change the relative orientations of the magnetizations of the source and drain between parallel and anti-parallel orientations. This technique is being used to study the mechanism of spin transport through organic semiconductors. The measurements were carried out using the Physical Properties Measurement System purchased with this grant. Cartoon of organic field effect transistor. The source/drain contacts, the gate contact and the dielectric are Co(400Å)/Au(20Å), doped Si(500μm)/Al(100Å)/Au(750Å) and SiO 2 (2850Å), respectively. The thickness of the tetracene single crystal is several thousand angstroms. The channel width and length are 1μm and 1000Å, respectively. The source/drain contacts have different geometries so as to have different coercive fields. VDVD VGVG Source Drain Channel (tetracene single crystal) DielectricGate ( R - R 0 )/ R 0 (%) Magnetic Field (gauss)

Education: This work is being carried out by Mr. Masaya Nishioka, a graduate student in the Physics Graduate Program at the University of Minnesota. The materials and devices are prepared with the support of the University of Minnesota MRSEC and the measurements are carried out using the Physical Properties Measurement System purchased under this program. Undergraduates also used this instrument. An REU student, Emily Beauvois, from Augsberg College retrofitted a UV source to the apparatus this past summer and was able to modulate the conductivity of an OSC. This will be incorporated in future magnetotransport measurements. Societal Impact: The device being studied is, in principle, a new transistor which could have a big impact on technology if it could be operated at room temperature. There are three new properties: first, the current can be modulated in two ways, by changing either the gate voltage or the relative magnetizations of the contacts. Second, the presence of two magnetic contacts gives the device memory. Third, the device could be on a flexible substrate. Because traditional transistors do not have these properties, variants of this device could change engineering practice. Magnetotransport Studies of Organic Spin Valves A. M. Goldman, University of Minnesota, DMR