N.L. Tran, J.Z. Sexton, T.J. Grassman, B. Fruhberger, A.C. Kummel University of California, San Diego S.V. Patel, T.E. Mlsna Seacoast Science AFOSR MURI#

Slides:



Advertisements
Similar presentations
Objective of the session.
Advertisements

Bellow valve (trap&pump) Inside glove box. (Note: Ar glove box is not necessary, if you work with single crystalline organic materials like rubrene that.
Overview of Vacuum Systems Tejas Deshpande 24 July, 2014.
1 Lorentz Force Tunneling Spectrometer for Studying Molecules on Single Crystal Surfaces Darin T. Zimmerman Brad A. Petrilla, John R. Rea, Darrell L. Sharp.
Wittenberg 2: Tunneling Spectroscopy
Auger Electron Spectroscopy of In 2 O on GaAs(001)-(2x4) As, Ga In O Ga As In:O = 2:1 In 2 O 3(s)  In 2 O (g) +O 2(g) Scanning Tunneling Microscopy and.
Applications: CO Gas Sensor
Pressure Sensors.
Platzhalter Bild Vacuum Transfer System for loading the Sartorius Prototype Mass Comparator CCL1007 Thomas Fehling, NCSLI-Conference, Washington D.C.,
MEMs Fabrication Alek Mintz 22 April 2015 Abstract
Internal Cryomodule Instrumentation Sensors, Actuators, Heaters, and Wiring ERL Main Linac Cryomodule 9/5/2012 Peter Quigley Internal Design Review.
PEEM III Endstation Design Review
Hydronic Mechanical Controls
AUSTEN K. SCRUGGS CALIFORNIA STATE UNIVERSITY, FRESNO RIMI FACILITY INSTRUMENTATION.
Aaron Vallett EE 518 April 5 th, 2007 Principles and Applications of Molecular Beam Epitaxy Instructor: Dr. J. Ruzyllo.
Gas and Liquid Metering. Why Metering? Measuring flow rate and cumulative volume Selling System Control Losses detection Reservoir outlets Pumping stations.
Scanning Probe Microscopy (SPM) Real-Space Surface Microscopic Methods.
L 17 - Thermodynamics [2] Today’s topics –Practical thermal effects –Devices for temperature measurement –Mechanisms of heat transfer Science dealing.
Pressure 1 atmosphere ~ 1 bar ~ 760 mm Hg ~ 760 torr ~ 100,000 Pa Ion gauges read in mbar i.e. 1x mbar = 1x atm. Sometimes ion gauges read.
Solar Cell conductive grid and back contact
L 17 - Thermodynamics [2] Science that studies the relationships between heat and work Science that studies the relationships between heat and work it.
Gas Chromatography Carrier Gas Flow Control Injector Port Column Column Oven Detector Recorder The GC system consists of gas supplies for the mobile phase.
LISA STUDIES AT THE UNIVERSITY OF COLORADO Michael J. Nickerson, Ellery B. Ames, John L. Hall, and Peter L. Bender JILA, University of Colorado and NIST,
Chromatography Separates components in mixture: Based on - polarity
Methods in Surface Physics Experimentation in Ultra-High Vacuum Environments Hasan Khan (University of Rochester), Dr. Meng-Fan Luo (National Central University)
1 L 17 - Thermodynamics [2] Science that studies the relationships between heat and work and the conversion of one into the other Science that studies.
Copyright © Texas Education Agency, All rights reserved. 1 Electronics The Nature of Matter.
Nano/Micro Electro-Mechanical Systems (N/MEMS) Osama O. Awadelkarim Jefferson Science Fellow and Science Advisor U. S. Department of State & Professor.
Chemical Bonding & the formation of Compounds
LCGT Cryogenics Status Report KEK T.Suzuki.
Center for Materials for Information Technology an NSF Materials Science and Engineering Center Vacuum Systems Lecture 6 G.J. Mankey
Nanonics CryoView 2000™ CryoView 2000™ Product Presentation.
S (LLV, 150 eV) and C (KLL, 265 eV) Auger peaks scale with varied TTPO coverage C peak loses significance in prolonged study as it is present following.
JCOV, 25 OCT 2001Thermal screens in ATLAS Inner Detector J.Godlewski EP/ATI  ATLAS Inner Detector layout  Specifications for thermal screens  ANSYS.
05 Novembre 2003Chamonix XIV Workshop, January How to deal with leaks in the QRL and magnet insulation vacuum Paul Cruikshank for AT/VAC Germana.
Department of Synchrotron Radiation Research Lund University
External forces from heat links in cryogenic suspensions D1, ICRR, Univ. Tokyo Takanori Sekiguchi GWADW in Hawaii.
Rotationally-Resolved Spectroscopy of the Bending Modes of Deuterated Water Dimer JACOB T. STEWART AND BENJAMIN J. MCCALL DEPARTMENT OF CHEMISTRY, UNIVERSITY.
Atomic-absorption spectroscopy
Junction Formation The position of the junction for a limited source diffused impurity in a constant background is given by The position of the junction.
56 MHz SRF Cavity Thermal Analysis and Vacuum Chamber Strength C. Pai
Removal of 3 He from 4 He (R&D) David Haase, Franklin Dubose, Travis McCaw and Paul Huffman North Carolina State University.
56 Mhz Vacuum Mike Mapes Mhz Insulating Vacuum TURBO PUMP WITH GATE VALVE AND GAUGE SET MOUNTED ON TANK SIMILAR TO RHIC CRYOSTAT & VALVE.
Solar Cells need a top side conductor to collect the current generated They also need a conductive film on the backside.
1 Vacuum chambers for LHC LSS TS Workshop 2004 Pedro Costa Pinto TS department, MME group Surface Characterization & Coatings Section.
University of Arkansas, Fayetteville Above right is a schematic diagram showing a top view of the UHV chamber for the two-tip low- temperature STM system.
Vacuum Studies of LHCb Vertex Locator Sensors Gwenaëlle Lefeuvre, Ray Mountain, Marina Artuso Department of Physics, Syracuse University Abstract : The.
Date 2007/Sept./12-14 EDR kick-off-meeting Global Design Effort 1 Cryomodule Interface definition N. Ohuchi.
-1- Steve Virostek (LBNL) and Li Wang (SINAP) Instrumentation for the MICE Coupling Coil Steve Virostek Lawrence Berkeley National Lab February.
Raffia Siddique National University of Sciences and Technology sector H-12 Islamabad
THERMAL ANALYSIS FOR PREFORMULATION TRIALS
Paul Frank Institute of Solid State Physics, Graz University of Technology Financially supported by the Austrian Science Fund.
EKT 451 CHAPTER 6 Sensor & Transducers.
Vacuum Systems for Electron Microscopy Constraints on Specimens Specimens placed in the electron microscope must be able to withstand very high vacuum.
Status of the FAIR CCC and Cryostat
Design of the Injection Can
T5.2: Harmonization - Material and Component Reference
SESAME: Surface Electric Sounding and Acoustic Monitoring Experiment
LARP Vertical Test Facility
ROX sensor packaging and mounting scheme for use on dilution STM sample plates Ben MacLeod Jan
External forces from heat links in cryogenic suspensions
FP420 Detector Cooling Thermal Considerations
Irradiation test of Pressure Transducers for the LHC machine
Example Design a B diffusion for a CMOS tub such that s=900/sq, xj=3m, and CB=11015/cc First, we calculate the average conductivity We cannot calculate.
FRESCA Cryostats Outer cryostat during pressure test at the manufacturer Top plate and lambda plate for the outer cryostat Inner cryostat during reception.
Determination of the thermal conductivity of a metal
a b c d Figure 1. Laboratory set-up for Experiment #3. CaCl2 CO2
Work Supported by NSF (DMR ) & Penn State University
Cryomodule Assembly Plan
Optical fiber based sensors for low temperature and superconductors
Presentation transcript:

N.L. Tran, J.Z. Sexton, T.J. Grassman, B. Fruhberger, A.C. Kummel University of California, San Diego S.V. Patel, T.E. Mlsna Seacoast Science AFOSR MURI# F Test Chamber Mass Flow Control Temperature Controlled Enclosure Heat Exchanger Flow Meter Data Acquisition And Control PC 4-Way Valve Temperature Controlled Bubblers Carrier Gas Exhaust Goal Determination of Material Growth and Analyte Interaction Evaluation of Sensor Performance DFT Computation Phthalocyanine Deposition Current Capabilities: In Preparation: Develop Instruments to: (a) Fabricate Metallo-Phthalocyanine (MPC) Chemically Sensitive Field Effect Transistor (ChemFet) (b) Test MPC ChemFETs (c) Image Sensor Materials  E binding of Cl 2 using GGA-DFT Binding Site[eV] DFT simulations can aid in the assignment of observed STM features Computation suggest multiple possible binding sites for Cl 2 (Cu and the organic ligand) Custom designed MBE cell for MPc deposition MBE cell capabilities include: fast introduction of different MPcs differential pumping H 2 O cooled Cu heat shield to minimize heat transfer and protect UHV instrumentation plate valve allowing separation between MBE cell and UHV chamber Low T effusion cell Linear & Linear/Rotary feedthroughs control plate valve Cu cooling shield braised onto SS can Two mounted tees to connect shafts to feedthroughs Two side ports for mounting turbo pump and ion gauge Effusion cell shutter Plate valve Cu spacers for heat transfer – also act as hard stops Linear feedthrough Cu plate Linear/rotary feedthrough Viton o-ring for sealing Closed to UHV Open to UHV And for deposition Low Temperature STM for Single Molecule Studies: funded by NSF Scanner: Beetle type with x-,y-coarse movement Cooling: Liquid He bath cryostat; Scanner 100% surrounded by a 4K shield Vibration isolation: Internal spring system with eddy current damping and external isolation with pneumatic isolation leg Additional shutter to control in-situ gas dosing at low temperature onto STM mounted sample Temperature variation either by heating the complete STM scanner or just the sample The Createc STM-SY combines a low-temperature STM (LT-STM) with three chambers: load-lock, sample preparation, and analysis. High Resolution Images of Complex Molecules At Low Temperature due to Extremely Stable Environment Instrument Features: - Additional He gas cooled radiation shield in between to improve the thermal isolation - Eddy current vibration damping of the pendulum motion of the inner cryostat - STM is completely isolated (thermally and electrically) when tunneling (a) 8K STM image of TBPP (porphyrin) on Cu(100), (b) STM simulation of TBPP/Cu(100); (c) structure of TBPP on Cu(100). Note the excellent submolecular resolution at the good agreement with the simulation. From Moresco et al 50 electrical feedthroughs Closed-loop temperature control: ± 0.05° C; 20 minute response time Closed-loop relative humidity control: % ± 2% RH; 10 minute response time Open-loop permanent gas concentration control: ± 4 ppm; 4 minute response time; or, Open-loop volatile organics concentration control: up to 8 volatile organics from temperature-controlled bubblers in any one experiment, 4 minute response time Temperature and humidity sensors inside chamber Outer enclosure with closed-loop temperature control: 25 ± 0.5°C Test runs are fully automated Room temperature STM Filled state image of CuPc on Au(111) at monolayer coverage Metal center of adsorbed CuPc appears dark, consistent with unfilled Cu-dz 2 orbitals Conditions: -1 V sample bias, 0.3 nA tunneling current 60 Å x 60 Å Future Plans Plate valve mechanics: Use STM to image growth modes and analyte binding sites for Metallo-Phthalocyanines Test sensors for ppb sensitivity and selectivity to Chemical Warfare Agent (CWA) simulants