行業(yè)標(biāo)準(zhǔn)，高性能CCD相機(jī)

PIXIS系列相機(jī)是集成度高，低噪聲設(shè)計(jì)的科學(xué)成像/光譜相機(jī)，響應(yīng)范圍從紫外到近紅外。結(jié)合PI的XP制冷技術(shù)，PIXIS是市場(chǎng)上的一款提供全金屬真空封存，深度制冷的科研級(jí)CCD相機(jī)。真空質(zhì)量終生質(zhì)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(shí)驗(yàn)中理想的選擇，例如：拉曼光譜，波什-愛因斯坦凝聚態(tài)（BEC），太陽(yáng)能器件檢測(cè)，熒光實(shí)驗(yàn)等等。

PIXIS相機(jī)可以選擇eXcelon鍍膜技術(shù)，增加其敏感度同時(shí)抑制近紅外波段的干涉現(xiàn)象。

PIXIS相機(jī)具有以下特點(diǎn):

• 支持不同芯片尺寸

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

• 獨(dú)特的全金屬真空封存技術(shù)

• 靈活的讀出設(shè)置

• 高速USB2.0接口

• 功能的 64位 LightField 操作平臺(tái)

PIXIS系列相機(jī)是高度集成化，低噪聲設(shè)計(jì)的科學(xué)成像/光譜相機(jī)，可應(yīng)用于紫外到近紅外各類實(shí)驗(yàn)。

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(jī)都提供了同類相機(jī)中的敏感度，的噪聲以及的動(dòng)態(tài)范圍。   

Images courtesy of Prof. Wolfgang Ketterle, MIT.

探測(cè)范圍180nm 至 1100nm:

可滿足各類實(shí)驗(yàn)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(qiáng)型CCD 或者 Unichrome/Lumogen phosphor鍍膜

結(jié)合eXcelon技術(shù)，提升相機(jī)的敏感度。

普林斯頓儀器獨(dú)特的真空封存技術(shù):

終生真空質(zhì)保

風(fēng)冷或者水冷均可達(dá)-90℃

長(zhǎng)時(shí)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(hù)

獨(dú)特 的eXcelon技術(shù)，用于背照型CCD:

增強(qiáng)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(xiàn)象

查看更多 eXcelon 的信息

雙讀出放大器:

增強(qiáng)的系統(tǒng)靈活性

高敏讀出放大器具有極低的讀出噪聲

大動(dòng)態(tài)讀出放大器增加了數(shù)據(jù)深度

高速USB2.0數(shù)據(jù)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(shù)據(jù)傳輸能力，可達(dá)2MHz讀出速度

LightField的64-位操作平臺(tái):

直觀易上手的用戶界面設(shè)計(jì).

內(nèi)置數(shù)學(xué)引擎，實(shí)時(shí)獲得圖像與光譜的數(shù)據(jù)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(duì)接.

IntelliCal 精準(zhǔn)的波長(zhǎng)校準(zhǔn)和強(qiáng)度校準(zhǔn)，一鍵完成。

用于成像和光譜學(xué)的PIXIS CCD相機(jī)型號(hào)比較和數(shù)據(jù)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 shown 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.