iStar门控探测器
Andor

iStar门控探测器

整合最优秀CCD & sCMOS芯片以及像增强器技术

最新
  iStar sCMOS
  • 超快帧速可达4,000 fps
  • 低噪声,高灵敏度
  • 简单易用,高度兼容
  • 小于2ns的高精度门控
  • 市场领先的全幅动态范围
sec

纳秒时间分辨应用

量子物理纠缠
等离子体诊断
激光击穿诱导荧光光谱
燃烧
非线性光学
时间分辨荧光



量子物理

即便距离非常远,当两个粒子保持关联时量子纠缠也会发生,从而一个粒子的行为也会影响另一个粒子。爱因斯坦光子纠缠现象描述为“鬼魅般的超巨作用”。量子纠缠研究是目前两个新兴领域量子计算和量子密码学的基础。

精准门控和高灵敏度的iStar sCMOS,为光子纠缠或非纠缠态研究提供了更高的分辨能力。

相关阅读
文章资料:通过量子纠缠成像拯救薛定谔的猫

选择适合您需求的

Fiber-optic coupling to sensor - maximum throughput Phosphor - conversion of photoelectroncs into green photons Micro Channel Plate (MCP) - photoelectroncs amplification Fast-gated photocatode and substrate
CCD&sCMOS传感器
门控
像增强探测器

iStar系列产品提供多种高分辨率的传感器以获得最清晰的图像和光谱特性,同时具有最高的动态范围。

iStar采用光纤锥直接耦合像增强器,以保证最大的搜集效率,这与透镜耦合受制于更低的通光量、成像晕影与变形不同。

型号 iStar CCD 312 iStar CCD 320 iStar CCD 334 iStar CCD 340 iStar sCMOS
像素矩阵 512 x 512 1024 x 256 1024 x 1024 2048 x 512 2560 x 2160
像素大小 24 26 13 13.5 6.5
高空间/光谱分辨率 - -
快速成像 - - -
高频光谱 -
窄带光谱
同时宽频光谱 - - -
延展多通道 - -

希望有更多的动态范围?

< 上一篇:得到更快!

比较读出噪声 比较动态范围

希望拥有更快的速度

> 下一篇:更大的动态范围!

持续的全帧速率 (fps) 最快连续光谱采样率

* 2x2融合(13微米PIX 。 ),有效1.4 MP

竞争对手联运ICCD : 1MP , 12.8微米像素尺寸

竞争对手emICCD : 100万像素, 13微米像素尺寸

模型选择

MODELS iStar CCD 312 iStar CCD 320 iStar CCD 334 iStar CCD 340 iStar sCMOS
Max Frame rate 15.8 fps 15.9 fps 4.2 fps 2.5 fps 50 fps *
Spectral rates
FVB
Crop mode / ROI
 
291
6,667
 
323
3,571
 
145
3,450
 
135
1,825
 
-
4,008
Pixel well depth 320,000 e- 500,000 e- 100,000 e- 100,000 e- 30,000 e-
Lowest read noise 5.4 e- 7 e- 5 e- 6 e- 2.6 e-
Min. dark current 0.25 e-/pix/s 0.2 e-/pix/s 0.1 e-/pix/s 0.1 e-/pix/s 0.18 e-/pix/s
Learn more SPEC SHEET SPEC SHEET SPEC SHEET SPEC SHEET SPEC SHEET
Contact Us

* 2x2 binning (13 µm pix.), effective 1.4 MP

客户出版物

Author Title Year
Portable Deep-Ultraviolet (DUV) Raman for Standoff Detection
Hybrid interferometric/dispersive atomic spectroscopy of laser-induced uranium plasma
Diesel ignition delay and lift-off length through different methodologies using a multi-hole injector
Classification of Chinese tea leaves using laser-induced breakdown spectroscopy combined with the discriminant analysis method
Synthesis and luminescent properties of Eu 3+/Eu 2+ co-doped calcium aluminosilicate glass–ceramics
Laser produced plasma diagnosis of carcinogenic heavy metals in gallstones
Generation of Antimicrobial NOx by Atmospheric Air Transient Spark Discharge
Laser-induced breakdown emission in hydrocarbon fuel mixtures
Analysis of benzoquinone decomposition in solution plasma process
Electron density measurements behind a hypersonic shock wave in argon
Propagation distance-resolved characteristics of filament-induced copper plasma
Setup for microwave stimulation of a turbulent low-swirl flame
Measurement of plasma electron density generated in an experiment of Laser Shock Processing, utilizing the Hα-line
Throwing light on hydroxyquinoline-based ruthenium sensitizers with long-lived charge carrier boosts photocatalytic H2 evolution
Comprehensive study on different crystal field environments in highly efficient NaLaF4:Er3+ up conversion phosphor
High-Sensitivity In-Situ Soot Particle Sensing in an Aero-Engine Exhaust Plume Using Long-Pulsed Fiber-Laser Induced Incandescence
Real-time imaging of spin-to-orbital angular momentum hybrid remote state preparation
Time-resolved detection of aromatic compounds on planetary surfaces by ultraviolet laser induced fluorescence and Raman spectroscopy
Transient absorption dynamics of sterically congested Cu (I) MLCT excited states
Temperature and water mole fraction measurements by time-domain-based supercontinuum absorption spectroscopy in a flame
Unveiling the identity of distant targets through advanced Raman-laser-induced breakdown spectroscopy data fusion strategies