行業標準，高性能CCD相機

PIXIS系列相機是集成度高，低噪聲設計的科學成像/光譜相機，響應范圍從紫外到近紅外。結合PI*的XP制冷技術，PIXIS是市場上*的一款提供全金屬真空封存，深度制冷的科研級CCD相機。真空質量終生質保。

高量子效率，超低噪聲電子電路，使得PIXIS成為高要求的低光實驗中理想的選擇，例如：拉曼光譜，波什-愛因斯坦凝聚態（BEC），太陽能器件檢測，熒光實驗等等。

PIXIS相機可以選擇eXcelon鍍膜技術，增加其敏感度同時抑制近紅外波段的干涉現象。

PIXIS相機具有以下特點:

• 支持不同芯片尺寸

• 頻譜響應從~ 180nm至~1100nm （紫外到近紅外）波段，更有eXcelon抗干涉技術eXcelon technology。

• 的全金屬真空封存技術

• 靈活的讀出設置

• 高速USB2.0接口

• 功能強大的 64位 LightField 操作平臺

PIXIS系列相機是高度集成化，低噪聲設計的科學成像/光譜相機，可應用于紫外到近紅外各類實驗。

PIXIS系列有前照型CCD，后照型CCD，后照深耗盡型CCD，適合成像或成譜的芯片格式。每一款PyLoN相機都提供了同類相機中的敏感度，的噪聲以及的動態范圍。   

Images courtesy of Prof. Wolfgang Ketterle, MIT.

探測范圍180nm 至 1100nm:

可滿足各類實驗需求

可選高于95%的量子效率

紫外波段的量子效率，可選擇紫外增強型CCD 或者 Unichrome/Lumogen phosphor鍍膜

結合eXcelon技術，提升相機的敏感度。

普林斯頓儀器的真空封存技術:

終生真空質保

風冷或者水冷均可達-90℃

長時間曝光下的超低暗噪聲

單層透射窗口增加芯片的敏感度

無需額外的維護

的eXcelon技術，用于背照型CCD:

增強的靈敏度，帶來更好的量子效率

減少背照式CCD的近紅外干涉現象

查看更多 eXcelon 的信息

雙讀出放大器:

增強的系統靈活性

高敏讀出放大器具有極低的讀出噪聲

大動態讀出放大器增加了數據深度

高速USB2.0數據接口:

任何電腦直接連接，無需額外硬件

即插即用

真正的16位數據傳輸能力，可達2MHz讀出速度

LightField的64-位操作平臺:

直觀易上手的用戶界面設計.

內置數學引擎，實時獲得圖像與光譜的數據分析.

PICAM（64）位通用程序語言，方便的程序修改與編譯.

與LabVIEW，MATLAB，EPICS等第三方軟件無縫對接.

IntelliCal 精準的波長校準和強度校準，一鍵完成。

用于成像和光譜學的PIXIS CCD相機型號比較和數據表

Imaging cameras (anchor link to table) | Spectroscopy cameras (anchor link to table)

Sensor Types:

Princeton Instruments' proprietary eXcelon process increases detector sensitivity in the blue and NIR while suppressing etalon interference fringes.

B/I DD (Back-illuminated deep depletion) sensors have up to 95% QE in the NIR with minimal etaloning.

B/I (Back-illuminated) sensors have up to 95% QE in the visible but are subject to etaloning in the NIR.

BUV (Enhanced UV) sensors offer the highest UV sensitivity with moderate visible sensitivity.

F/I (Front-illuminated) CCD sensors offer economical performance from ~400-1000 nm with up to ~50% QE and negligible etaloning. Open Electrode architecture improves QE by reducing the area of the electrodes.

Pixel Size:

All PIXIS cameras offer 99% fill factors

Larger pixels offer higher well capacity

Smaller pixels offer higher spatial resolution in some cases; for more information, see hyperlink to IsoPlane page

Peak QE:

Maximum values of quantum efficiency (QE) are n at 25° C.

Tip-Enhanced Raman Spectroscopy

TERS - Tip-Enhanced Raman spectroscopy

Fluorescence, Phosphorescence, and Photoluminescence Spectroscopy

Fluorescence, phosphorescence and photoluminescence occur when a sample is excited by absorbing photons and then emits them with a decay time that is characteristic of the sample environment.

Astronomical Imaging

Astronomical imaging can be broadly divided into two categories: (1) steady-state imaging, in which long exposures are required to capture ultra-low-light-level objects, and (2) time-resolved photometry, in which integration times range from milliseconds to a few seconds.

General Raman

The most common application of Raman spectroscopy involves the vibrational energy levels of a molecule. Incident laser light in the UV, visible or NIR, is scattered from molecular vibrational modes.

Surface-Enhanced Raman Spectroscopy

SERS - Surface-enhanced Raman spectroscopy

Bose-Einstein Condensate

Bose-Einstein condensate (BEC) can be regarded as matter made from matter waves. It is formed when a gas composed of a certain kind of particles, referred to as “bosonic” particles, is cooled very close to absolute zero.

Coherent Anti-Stokes Raman Spectroscopy

Coherent Anti-Stokes Raman spectroscopy (CARS) a type of non-linear Raman spectroscopy. Instead of the traditional single laser, two very strong collinear lasers irradiate a sample.

Stimulated Raman Scattering

Stimulated Raman scattering takes place when an excess of Stokes photons that were previously generated by normal Raman scattering are present or are deliberately added to the excitation beam.

Micro-Computed Tomography

Micro Computer Tomography is a unique technique for the noninvasive, nondestructive 3D characterization of materials down to a micrometer scale.