Spectroscopy EMCCD Detector - Newton 970 EMCCD
Andor

Newton 970

Newton 970 offers Unrivalled EMCCD performance for spectroscopic applications. It utilizes a 1024 x 255 or 2048 x 512 array of 26 μm or 13.5 μm pixels, with thermoelectric cooling down to -100°C, resulting in negligible dark which provides unrivalled performance.

  • EM sensor
  • Multi-Megahertz Readout
  • TE cooling to -100°C
  • UltraVac™
  • 16 x 16 μm pixel size

Overview

EM technology enables charge from each pixel to be multiplied on the sensor before readout, providing single photon sensitivity. The Newton EM platform combines a 1600 x 200 (or 1600 x 400) array of 16 μm pixels, thermoelectric cooling down to -100°C for negligible dark current, 3MHz readout and USB 2.0 plug-and-play connectivity to provide unrivalled performance for spectroscopic applications. The dual output amplifiers allow software selection between either a conventional High Sensitivity or Electron Multiplying outputs to suit a broad range of photon regime conditions. This makes the Newton EMCCD the ideal choice for ultrafast chemical mapping applications e.g. SERS, TERS or luminescence mapping.

Specifications

Key Specifications
Sensor Options BV: Back Illuminated CCD, Vis-optimized
BVF: Back Illuminated CCD, Vis-optimized and antifringing
FI: Front Illuminated CCD
UV: Front Illuminated CCD with UV coating
UVB: Back Illuminated CCD with UV coating
Active Pixels 1600 x 200
Pixel Size 16 x 16 μm
Image area 25.6 x 3.2 mm with 100% fill factor
Minimum Temperature Air Cooled -80°C
Coolant recirculator -95°C
Coolant chiller, coolant @ 10ºC, 0.75 l/min -100°C
Max spectra per second 649 (Full Vertical Bin), 1,515 (Crop Mode - 20 rows)
System window type Single UV-grade fused silica window, uncoated. Various AR coatings & MgF2 options available
Blemish specifications Grade 1 as per sensor manufacturer definition

Features and Benefits

Features Benefits
EM sensor technology <1e- read noise
Fringe suppression technology as standard (970-BVF only) Fringing minimized for NIR applications
Multi-Megahertz Readout High repetition rates achievable with low noise electronics
TE cooling to -100°C Negligible dark current without the inconvenience of LN2
UltraVac™ Permanent vacuum integrity, critical for deep cooling
16 x 16 μm pixel size Optimized pixel size for achievement of high resolution
Dual output amplifiers Software select between either a conventional High Sensitivity output (for low light applications) or an Electron Multiplying output (for single photon sensitivity
Crop Mode Operation Achieve the highest possible spectral rates of over 1,500 spectra per second
Simple USB Connection USB connection direct from back of camera – no controller box required! 
Solis software for Spectroscopy Comprehensive, user-friendly interface for simultaneous detector & spectrograph control
Software Development Kit (SDK) Ease of control integration into complex setups: Matlab, Labview, Visual Basic or C/C++

Graphs

Graphs and Drawings
QE Curve
 

Dark Current
 
Readout Rate & Speed

Dimensions - Front 

Dimensions - Top
 
Dimensions - Side

Connector Panel

Typical Setup

Learning

The Andor Learning Center hosts a wide range of case studies, technical articles and webinars to guide you through the many features of our portfolio.

Gallery

Papers

AuthorTitle
Raman Microspectroscopy – A Non-Invasive Analysis Tool For Monitoring Of Collagen-Containing Extracellular Matrix Formation in a Medium-Throughput Culture System
Time-lapse Raman imaging of single live lymphocytes
Au Nanowire-on-Film SERRS Sensor for Ultrasensitive Hg2+ Detection
Simultaneous determination of the composition and temperature gradients in the vicinity of boiling bubbles in liquid binary mixtures using one-dimensional Raman measurements
Microspectroscopic Analysis of Green Fluorescent Proteins Infiltrated into Mesoporous Silica Nanochannels
MicroRaman spectroscopy of diamond and graphite in Almahata Sitta and comparison with other ureilites
Interactions of Perylene Bisimide in the One-Dimensional Channels of Zeolite L
Effects of ethanol, formaldehyde, and gentle heat fixation in confocal resonance Raman microscopy of purple nonsulfur bacteria
Doppler and Stark Broadenings of Spectral Lines of Highly Excited Helium Atoms for Measurement of Detached Recombining Plasmas in MAP-II Divertor Simulator
Defining CYP3A4 Structural Responses to Substrate Binding. Raman Spectroscopic Studies of a Nanodisc-Incorporated Mammalian Cytochrome P450
Synthesis, structure and high temperature Mössbauer and Raman spectroscopy studies of Ba1.6Sr1.4Fe2WO9 double perovskite
Synthesis, Rietveld refinements and Raman spectroscopic studies of tricationic lacunar apatites Na1-xKxPb4(AsO4)3 (0 x 1)
Hierarchical Cluster Analysis (HCA) of Microorganisms: An Assessment of Algorithms for Resonance Raman Spectra
Solution processed ZnO nanowires/polyfluorene heterojunctions for large area lightening
Crystal chemistry, Rietveld refinements and Raman spectroscopy studies of the new solid solution series: Ba3 xSrx(VO4)2 (0 x 3)
Observation of spontaneous Bose-Einstein condensation of excitons at sub-Kelvin temperatures
Observation of ArF laser induced structural defects in highly transparent synthetic silica glass
Gas temperature and electron density profiles in an argon dc microdischarge measured by optical emission spectroscopy
Elucidation of the internal physical and chemical microstructure of pharmaceutical granules using X-ray micro-computed tomography, Raman microscopy and infrared spectroscopy
Time-Resolved Light Emission of a Cathode Spot Ignited in Vacuum and under Plasma

Drivers and Downloads

DOWNLOAD NOW

Newton Spectroscopy EMCCD Series
EM technology enables charge from each pixel to be multiplied on the sensor before readout, providing single photon sensitivity with up to 3 Megahertz readout and USB connectivity. The camera utilizes a 1600 x 400 (or 200) array of 16 μm pixels with thermoelectric cooling down to -100°C resulting in negligible dark current and provides unrivalled performance for spectroscopic applications. The dual output amplifiers allow software selection between either a conventional CCD or Electron Multiplying outputs (1016 R2).