Camere intensificate per applicazioni di Imaging e Spettroscopia risolte nel tempo
Camere intensificate Serie iStar da Oxford Instruments AndorLe camere ICCD Serie iStar di Oxford Instruments Andor sono dotate di sensori CCD di grado scientifico accoppiati ad un intensificatore di immagine di alta qualità e con elettronica di controllo del fotocatodo estremamente veloce.
L’intensificatore di immagine si comporta come se fosse uno shutter ottico ultra-veloce con exposure time dell’ordine del nanosecondo. Grazie all’elevato guadagno dell’intensificatore, inoltre, le camere ICCD Andor sono in grado di rilevare facilmente segnali estremamente deboli fino al singolo fotone.
I modelli iStar 320 e 340 sono dotati di sensore rettangolare rispettivamente di 1024x255 pixels da 26 µm e 2048x512 pixels da 13.5 µm e sono impiegati principalmente in applicazioni di Spettroscopia. I modelli iStar 312 e 334 prevedono invece sensori quadrati, rispettivamente di 512x512 pixels da 24 µm e 1024x1024 pixels da 13 µm, e sono pertanto tipicamente impiegati in applicazioni di Imaging, sebbene il modello iStar 334 sia comunemente utilizzato anche in Spettroscopia.
I modelli iStar 312, iStar 334 e iStar sCMOS prevedono invece sensori quadrati, rispettivamente di 512x512 pixels da 24 µm, 1024x1024 pixels da 13 µm e 2560x2160 pixels da 6.5 µm, e sono pertanto tipicamente impiegati in applicazioni di Imaging, sebbene il modello iStar 334 sia molto spesso utilizzato anche in Spettroscopia con particolare riferimento ad applicazioni LIBS in combinazione allo spettrografo Andor Mechelle.
- Gating con risoluzione temporale < 2 ns
- Ampio range di selezione del fotocatodo per applicazioni UV, VIS e NIR
- Repetition Rate del fotocatodo fino a 500 KHz
- Digital Delay Generator (DDG) integrato e completamente controllato via software
- Sistema di raffreddamento termoelettrico con temperatura minima raggiungibile di -40 °C (dark cur rent trascurabile)
Maggiori informazioni
Le camere ICCD Andor iStar 320 e 340 sono progettate per offrire la migliore soluzione oggi disponibile per applicazioni di Spettroscopia risolta nel tempo con scala del nanosecondo e ad alta risoluzione. L’aspect ratio 4:1 di tali sensori si adatta perfettamente all’impiego con gli spettrografi Andor Czerny-Turner Serie Shamrock ed i relativi accessori.
Il readout rate multi-MHz permette acquisizioni con spectra rate dell’ordine dei centinaia di spettri al secondo. Modalità di acquisizione speciali (Crop Mode e Fast Kinetics) sono inoltre implementate per consentire applicazioni di Spettroscopia molto rapide con spectra rate oltre i 1.000 ed i 10.000 sps, rispettivamente.
Le camere ICCD Andor iStar 312 and 334 con sensore quadrato sono progettate per offrire la migliore soluzione oggi disponibile per applicazioni di Imaging risolto nel tempo con scala del nanosecondo e ad alta risoluzione.
La iStar 334 è il modello più versatile, adatto sia ad applicazioni di Spettroscopia che di Imaging, ed è il detector impiegato con lo spettrografo Andor Mechelle con tecnologia Echelle in applicazioni di Laser Induced Breakdown Spectroscopy (LIBS).
L’ampia gamma di intensificatori di immagine di Generazione 2 e 3, con possibilità di scelta sia per la finestra in ingresso che per il tipo di fosforo, soddisfa qualsiasi requisito sul range di sensibilità, tra 120 nm e 1.100 nm, offrendo un gating time fino a < 2ns.
Tutte le camere Andor iStar sono dotate di interfaccia USB 2.0, che ne consente l’utilizzo anche con PC laptop, e di Digital Delay Generator (DDG) completamente integrato e controllato via software.
Questo consente una perfetta integrazione della camera iStar in esperimenti complessi con un’eccellente accuratezza nella sincronizzazione dei vari componenti che li costituiscono e con controllo del guadagno attraverso un'unica e semplice interfaccia interattiva.
Specifiche
Applicazioni
Downloads
Video
Opinioni degli utenti
Title | Author(s) | Institute | Year | Detector/Spectrograph |
---|---|---|---|---|
Plasma, Discharge | ||||
Invasiveness of high-power ns and ps pulsed laser beams on a ns pulsed N2 atmospheric pressure plasma jet | T. Keur, A. Limburg, S. Nijdam | Eindhoven University of Technology, Department of Applied Physics, The Netherlands | 2021 | iStar DH334T-18U-E3 |
Measuring the phase velocity of plasma waves using the double-image mode of the iStar-sCMOS | J. Held, S. Thiemann-Monjé | Chair for Experimental Physics II, Ruhr-Universität Bochum, Germany | 2021 | iStar-sCMOS-18U-E4 |
Measurement of photoluminescence from quantum dots interacting with a low-pressure plasma | J. Beckers, Z. Marvi, M. Hasani, T. Donders, G. Klaassen | Eindhoven University of Technology, | 2021 | iStar DH334T-18U-A3 |
The optimization of the Pockels-based Mueller polarimetry technique through overdetermination | A. Sobota1, H. Philpott1, O. Guaitella1, E. Garcia-Caurel2 | 1Eindhoven University of Technology, Department of Applied Physics, The Netherlands, 2Ecole Polytechnique Paris, France | 2021 | iStar DH334T-18U-73 |
Optical emission spectroscopy of a HiPIMS plasma | J. Held V. Schulz-von der Gathen | Chair for Experimental Physics II, Ruhr-Universität Bochum, Germany | 2018 | iStar DH320T-25U-A3 |
Feasibility study of passive high resolution optical emission spectroscopy for the electric field measurements in IShTAR | A. Kostic1,2, K. Crombé1,3, R. D’Inca2, J. Jacquot2, R. Ochoukov2, A. Nikiforov1, M. Usoltceva1,2,4, E. H. Martin5, J.-M. Noterdaeme1,2, and the IShTAR team | 1 Ghent University, Department of Applied Physics, Ghent, Belgium 2 Max-Planck-Institut für Plasmaphysik, Garching, Germany 3 LPP-ERM-KMS, TEC partner, Brussels, Belgium 4 Université de Lorraine, Nancy, France 5 Oak Ridge National Laboratory, Oak Ridge, Tennessee, USA | 2017 | iStar DH334T-18U-E3 Shamrock SR-750-B2 |
Automated 2D elemental mapping by Laser-Induced Breakdown Spectroscopy | G. Cairns1, J. Kaiser2 | 1Andor Technology, Belfast, United Kingdom 2Institute of Physical Engineering, Brno University of Technology, Czech Republic | 2014 | iStar DH734i-18F-031 |
Laser induced breakdown spectroscopy of Copper Indium Gallium Selenide (CIGS) thin film solar cells | D. Bartl | Robert Bosch GmbH, Corporate Sector Research and Advance Engineering Stuttgart, Germany | 2013 | iStar DH340T-18U-E3 |
Imaging of laser-induced plasma species | M. Bator, C. W. Schneider, T. Lippert | Paul Scherrer Institute, Department General Energy, Villigen PSI, Switzerland | 2013 | iStar DH334T-18F-03 |
Time-resolved detection of Hydrogen in steel products | R. Hergenröder | Department of Interface Processes, Leibniz-Institute for Analytical Sciences - ISAS, Dortmund, Germany | 2013 | iStar DH720-18F-033 |
High-speed measurements of the electron beam size at KARA | B. Kehrer1, N. Hiller1,2, P. Schütze3, E. Bründermann1, A. Müller1 | 1 KIT, Karlsruhe, Germany, 2 PSI, Villingen, Switzerland, 3 DESY, Hamburg, Germany | 2018 | iStar DH340T-18U-03 |
High sensitivity imaging of Thomson scattering signal | S. Hübner, J. Palomares, J. J. A. M. van der Mullen | Department of Applied Physics, Eindhoven University of Technology, The Netherlands | 2011 | iStar DH734-18U-631 |
Light emission profiles of a parallel plate dc micro discharge in different discharge modes | I. Stefanovic | Eperimental Physics II, University of Bochum, Germany | 2011 | iStar DH734-18F-031 |
Time-resolved optical emission spectroscopy of HiPIMS | V. Stranak, R. Hippler | Institute of Physics, University of Greifswald, Germany | 2009 | iStar DH740i-18U-032 |
Fast Imaging of the Atmospheric Pressure Glow Discharge | M. C. M. van de Sanden | Department of Applied Physics, University of Technology Eindhoven, The Netherlands | 2009 | iStar DH734-18U-031 |
Plasmadiagnostik an Radikalen und Metastabilen mit Hilfe der laserinduzierten Fluoreszenz | J. Barz | Fraunhofer Institut für Grenzflächen- und Bioverfahrenstechnik, Stuttgart, Deutschland | 2007 | iStar DH734i-18F-031 |
Application of an Echelle spectrometer for 2D mapping of aluminum alloy surfaces using MicroLIBS | M.T. Taschuk1, M. Tripathi2, A. Hanvey3, R. Al-Wazzan3, Y.Y. Tsui1 and R. Fedosejevs1 | 1 Department of Electrical and Computer Engineering, University of Alberta, Edmonton, Canada, 2 Andor Technology, S. Windsor, USA , 3 Andor Technology, Belfast, United Kingdom | 2007 | iStar DH734-18U-131 |
Zeitaufgelöste Spektroskopie von Glimmentladungen | F. Olcaytug | Institut für Mikrosystemtechnik, Universität Freiburg, Deutschland | 2007 | iStar DH720i-18U-053 |
Detection of Manganese in Sea Water Using Laser Induced Breakdown Spectroscopy | S. Koch, W. Garen, W. Neu | Faculty of Technology, University of Applied Science, Emden, Germany | 2004 | iStar DH734-25F-031 |
Fluorescence, Luminescence | ||||
Determination of triplet energies and decay times of light-emitting layers | S. Brüninghoff | Dept SO-ACP-7, Merck KGaA, Darmstadt, Germany | 2015 | iStar DH320T-18F-03 |
Influence of the speciation of uranium on transfer factors measured by Time-Resolved Laser-induced Fluorescence Spectroscopy (TRLFS) | F. Tawussi, L. Lütke, C. Walther | Institute for Radioecology and Radiation Protection, University of Hannover, Germany | 2014 | iStar DH334T-18F-A3 |
Spektroskopie hochgeladener Ionen in einer kryogenen Paul- Falle | L. Schmoeger, O. Versolato, B. Piest | Max-Planck-Institut für Kernphysik, Heidelberg, Deutschland | 2013 | iStar DH740-18U-032 |
High Enthalpy Flow Visualization using Laser Induced Fluorescence of Nitric Oxide | M. Kirschner, T. Sander, C. Mundt | Institute of Thermodynamics, University of the Federal Armed Forces Munich, Neubiberg, Germany | 2013 | iStar DH334T-18F-E3 |
Determination of fluorescence lifetimes of solvated Eu(III) and Cm(III) ions using Time-Resolved Laser Fluorescence Spectroscopy (TRLFS) | B. B. Beele1,2, C. M. Ruff2, T. Rabung 2, P. J. Panak1,2 | 1Radiochemistry, University of Heidelberg, Germany 2Institute for Nuclear Waste Disposal, Karlsruhe Institute of Technology, Germany | 2012 | Star DH734-18F-631 |
Laser induced fluorescence for detecting residual impurities in optical thin films at 193 nm excitation | C. Mühlig | Institute of Photonic Technology, Jena, Germany | 2011 | iStar DH740i-18F-032 |
Luminescence dynamics of a photosensitizer in a photocatalytic model system | S. Göde | Institute of Physics, University of Rostock, Germany | 2010 | iStar DH740i-18U-052 |
Phosphoreszenz in organischen Halbleitern | A. Köhler | Experimental Physics II, University of Bayreuth, Germany | 2008 | iStar DH734-18F-C31 |
Laserinduzierte Fluoreszenz (LIF) zur Untersuchung der Defektkinetik in hochreinen synthetischen Quarzgläsern | C. Mühlig | Leibniz Institut für Photonische Technolgien, Jena, Deutschland | 2007 | iStar DH734-18F-031 Oriel Instruments MS260i |
Plasmadiagnostik an Radikalen und Metastabilen mit Hilfe der laserinduzierten Fluoreszenz | J. Barz | Fraunhofer Institut für Grenzflächen- und Bioverfahrenstechnik, Stuttgart, Deutschland | 2007 | iStar DH734i-18F-031 |
Synchrotron, Free Electron Laser | ||||
Spectrotemporal manipulation of ultrashort pulses at the synchrotron light source DELTA | S. Khan, C. Mai, A. Meyer auf der Heide, P. Ungelenk | Zentrum für Synchrotronstrahlung (DELTA), Technische Universität Dortmund, Germany | 2018 | iStar DH334T-18U-E3 |
High-speed measurements of the electron beam size at KARA | B. Kehrer1, N. Hiller1,2, P. Schütze3, E. Bründermann1, A. Müller1 | 1 KIT, Karlsruhe, Germany, 2 PSI, Villingen, Switzerland, 3 DESY, Hamburg, Germany | 2018 | iStar DH340T-18U-03 |
Characterization of ultrashort and coherent VUV pulses at the DELTA storage ring | S. Khan1, F. H. Bahnsen1, M. Bolsinger1, S. Hilbrich1, M. Höner1, H. Huck1,2, M. Huck1, M. Jebramcik1, C. Mai1, A. Meyer auf der Heide1, R. Molo1, H. Rast1, G. Shayeganrad1, P. Ungelenk1 | 1 Zentrum für Synchrotronstrahlung (DELTA), Technische Universität Dortmund, Germany 2 now at Deutsches Elektronen-Synchrotron (DESY), Zeuthen, Germany | 2015 | iStar DH334T-18U-E3 |
Measurement of alkali metal vapor density using interferometric methods for the proton driven wakefield accelerator at CERN | F. Batsch, P. Muggli, E. Öz | Max Planck Institute for Physics, Munich, Germany | 2014 | iStar DH334T-18F-73 |
Spatial and spectral measurements of transition radiation emitted by an energetic electron bunch accelerated in a laser-driven plasma wakefield | C. Palmer, L. Schaper | Plasma Accelerator Group, DESY, Hamburg, Germany | 2013 | iStar DH334T-18U-03 |
In-situ Pulse Laser Heating in Diamond Anvil Cells with time-resolved temperature measurements | Z. Konôpková1, H.-P. Liermann1, W. Morgenroth2 | 1Extreme Conditions Beamline, PETRA III, DESY, Hamburg, Germany 2Institute of Geoscience, Goethe University of Frankfurt/Main, Germany | 2013 | iStar DH320T-18U-73 |
Single Shot Spectral Charcterisation of a SASE Free Electron Laser | M. Martins, M. Wellhöfer, J. T. Hoeft, W. Wurth | Institute of Experimental Physics, Unversity of Hamburg, Germany | 2007 | iStar DH740-18F-632 |
Semiconductor | ||||
Determination of triplet energies and decay times of light-emitting layers | S. Brüninghoff | Dept SO-ACP-7, Merck KGaA, Darmstadt, Germany | 2015 | iStar DH320T-18F-03 |
Orts- und zeitaufgelöste Spektroskopie an dichten Exzitonen | R. Schwartz | Institute of Physics, University of Rostock, Germany | 2010 | iStar DH740-18U-632 |
Phosphoreszenz in organischen Halbleitern | A. Köhler | Experimental Physics II, University of Bayreuth, Germany | 2008 | iStar DH734-18F-C31 |
Photovoltaics | ||||
Time-resolved photoluminescence of methylammonium lead triiodide (MAPbI3) films | M. C. Scharber | Linz Institute of Organic Solar Cells, Johannes Kepler University Linz, Austria | 2019 | iStar DH320U-18U-73 |
Laser induced breakdown spectroscopy of Copper Indium Gallium Selenide (CIGS) thin film solar cells | D. Bartl | Robert Bosch GmbH, Corporate Sector Research and Advance Engineering Stuttgart, Germany | 2013 | iStar DH340T-18U-E3 |
Probing time resolved charge- transfer-excition recombination in organic solar cells by time- gated spectroscopy | E. Da Como | Department of Physics and Center for Nanoscience (CeNS), Ludwig-Maximilian University Munich, Germany | 2011 | iStar DH740-18U-932 |
Delayed emission of charge transfer states in organic solar cells | F. Laquai | Max-Planck-Institute for Polymer Research, Mainz, Germany | 2010 | iStar DH740-18U-732 |
Quantum Optics | ||||
Low-intensity double-slit experiment for physics education and outreach | S. Barz, N. Hauser | Institute for Functional Matter and Quantum Technologies, University of Stuttgart, Germany | 2021 | iStar DH334T-18H-13 |
Real-time imaging of quantum entanglement | R, Fickler1,2, M. Krenn1,2, R. Lapkiewicz1,2, S. Ramelow1,2,3, A. Zeilinger1,2 | 1Vienna Center for Quantum Science and Technology, Faculty of Physics, University of Vienna, Austria 2Institute for Quantum Optics and Quantum Information, Austrian Academy of Sciences, Vienna, Austria 3Cornell University, Ithaca, USA | 2014 | iStar DH334T-18F-03 |
Liquid | ||||
Triplet solvation dynamics in hydrogen bonding liquids in hard and soft confinements | V. Talluto1, C. Böhmer1, T. Walther1, T. Blochowicz2 | 1Institute of Applied Physics, Technical University Darmstadt, Germany 2Institute of Condensed Matter Physics, Technical University Darmstadt, Germany | 2013 | iStar DH340T-18F-03 |
Biophysics | ||||
Photocycle Kinetics | R. Hagedorn | Institute of Biology, Humboldt University Berlin, Germany | 2009 | iStar DH734-18F-A31 |
Remarks:
1iStar 734 replaced by iStar 334
2iStar 740 replaced by iStar 340
3iStar 720 replaced by iStar 320
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