顕微鏡用サイエンティフィックCCDカメラ、8メガピクセル

ThorCam™

ThorCamは強力な画像取得ソフトウェアパッケージで、当社のカメラを32ビット版または64ビット版のWindows^®7または10で使用できるように設計されています。直観的で使いやすいグラフィカルインターフェイスによるカメラ制御や、イメージの取得・再生が可能です。シングルイメージキャプチャとイメージシーケンスをサポートしています。ソフトウェアの基本的な機能については、下記のスクリーンショットをご覧ください。

アプリケーションプログラミングインターフェイス(API)とソフトウェア開発キット(SDK)が付属しているため、OEMや開発者向けのカスタム用途にもお使いいただけます。SDKは、C、C++、C#、Python、Visual Basic .NETなど幅広いプログラミング言語に対応しています。また、LabVIEW、MATLAB、µManager*などのサードパーティソフトウェアパッケージもサポートしています。またブレイクアウトボードTSI-IOBOB2用のArduinoのコード例もご提供しています。

*µManagerによる制御は、現在はZelux および1.3 MP Kiraluxカメラではサポートされていません。Kiralux偏光検出型カメラをµManagerで操作した場合、取得できるのは強度画像のみです。偏光情報を含めた画像を生成するにはThorCamソフトウェアを使用する必要があります。

ソフトウェア

バージョン3.5.1

下のボタンをクリックしてThorCamソフトウェアのページにアクセスしてください。

ボードTSI-IOBOB2用のArduinoコードの例

下のボタンをクリックしてArduino用シールドTSI-IOBOB2のサンプルプログラムのダウンロードページにアクセスしてください。サンプルプログラムは3種類ご用意しております。

• 1 Hzのレートでカメラをトリガする
• 最大レートでカメラをトリガする
• ArduinoからのダイレクトAVRポートマッピングを使用してカメラの状態やトリガ取得をモニタする

色付きの枠で囲まれた部分をクリックするとThorCamの特長がご覧いただけます。

カメラ制御およびイメージ取得

カメラ制御およびイメージ取得機能は、ウィンドウの上にあるアイコン(上の画像中のオレンジの枠内)から実行できます。カメラパラメータの設定は、ツールアイコンをクリックすると表示されるポップアップウィンドウ内で行えます。スナップショットボタンを押すと、現在のカメラ設定を使用したシングルイメージが取得できます。

キャプチャスタート/ストップボタンを押すと、トリガイメージなどのカメラ設定に基づいたイメージキャプチャを開始します。

時系列および像系列のレビュー

図1のような時系列制御により、低速度画像の記録ができます。画像の総数とキャプチャ間の遅延時間を設定してください。出力結果は、高精度の無修正画像データとして保存するために、マルチページTIFFファイルとして保存されます。ThorCam内で、画像のシークエンス再生やフレームごとのコマ送り再生が可能です。

測定および注釈機能

上の画像の黄色い枠内にあるように、ThorCamには注釈および測定機能が多数内蔵されています。これは取得後の画像を分析する際に役立ちます。直線、長方形、円およびフリーハンドによる図形を画像上に描くことができます。注釈マークを付けた位置には文字を入力できます。また、測定モードでは対象とする2点間の距離を計測できます。

上の画像内の赤、緑、青の枠で囲まれた部分に、ライブ画像および取得済み画像に関する情報を表示させることができます。

ThorCamには計数機能も内蔵されており、画像内の対象点に印をつけてその数を計数することができます(図2参照)。画像の中心に固定されている十字のターゲットが基準点となります。

サードパーティアプリケーションおよびサポート

ThorCamは、LabVIEW、MATLAB、.NET.などのサードパーティソフトウェアパッケージもサポートしています。LabVIEWとMATLABは32ビット版ならびに64ビット版の両方をサポートいたします。当社カメラに付属する解説付きのフル機能APIを使えば、カメラを効率的にフルカスタマイズできます。

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図1:1秒間隔で撮影された10枚の時系列画像が、マルチページTIFFファイルとして保存されます。

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図2: ThorCamソフトウェアのスクリーンショット。計数機能によって画像内の3地点がマークされています。測定機能によって左下の直線が付加されています。直線の上には対象点間の距離がピクセル単位で表示されています。

性能に関する注意点

イメージシーケンスをディスクに保存するときに、システム性能が十分でないと「フレーム落ち」が発生する可能性がありますのでご注意ください。ホストシステムがカメラの出力データストリームを処理する能力は、ホストシステムの様々な特性に依存します。なお、USBハブを使用すると性能に影響を与える可能性があります。PCとは専用のケーブルで接続することをお勧めいたします。USB 2.0による接続はサポートされておりません。

まず、カメラのフレームレートと、ホストPCが画像を表示する能力およびフレーム落ちせずにディスクにストリーミングする能力とを区別することが重要です。カメラのフレームレートは露光および読み出し(例えば、クロックやROI)パラメータに依存します。ユーザによって設定された画像取得パラメータに基づいて、カメラのタイミング機能はデジタルカウンタのように動作し、1秒間にある特定の数のフレームを生成します。画像を表示するときは、このデータがPCのグラフィックシステムによって処理され、画像や動画を保存するときにはディスクに転送されます。この時、ハードドライブの速度が十分でないとフレーム落ちが発生します。

この問題に対する解決策の一つとして、ソリッドステートドライブ(SSD)のご使用をお勧めいたします。PCのそれ以外の仕様が十分であれば、多くの場合はこれによって解決します。SSDへの書き込み速度は、データのスループットを処理するのに十分なものでなければなりません。

大きなフォーマットの画像を早いフレームレートで処理する場合には、より速いスピードが必要な場合があります。その場合は、複数のSSDを用いてRAID0を構成するか、あるいはRAMドライブを使うといった方法が考えられます。後者の方法では保存スペースがPC上のRAMで制限されてしまいますが、実現可能な方法としては最も高速なものです。ImDiskは、無料のRAMディスク作製用ソフトウェアパッケージの一例です。RAMドライブは揮発性メモリであることにご注意ください。従って、データの損失を防ぐために、PCを再起動またはシャットダウンする前に、必ずデータをRAMドライブから不揮発性のハードドライブに移動させることが重要です。

Insights into Mounting Lenses to Thorlabs' Scientific Cameras

Scroll down to read about compatibility between lenses and cameras of different mount types, with a focus on Thorlabs' scientific cameras.

• Can C-mount and CS-mount cameras and lenses be used with each other?
• Do Thorlabs' scientific cameras need an adapter?
• Why can the FFD be smaller than the distance separating the camera's flange and sensor?

Click here for more insights into lab practices and equipment.

Can C-mount and CS-mount cameras and lenses be used with each other?

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Figure 1: C-mount lenses and cameras have the same flange focal distance (FFD), 17.526 mm. This ensures light through the lens focuses on the camera's sensor. Both components have 1.000"-32 threads, sometimes referred to as "C-mount threads".

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Figure 2: CS-mount lenses and cameras have the same flange focal distance (FFD), 12.526 mm. This ensures light through the lens focuses on the camera's sensor. Their 1.000"-32 threads are identical to threads on C-mount components, sometimes referred to as "C-mount threads."

The C-mount and CS-mount camera system standards both include 1.000"-32 threads, but the two mount types have different flange focal distances (FFD, also known as flange focal depth, flange focal length, register, flange back distance, and flange-to-film distance). The FFD is 17.526 mm for the C-mount and 12.526 mm for the CS-mount (Figures 1 and 2, respectively).

Since their flange focal distances are different, the C-mount and CS-mount components are not directly interchangeable. However, with an adapter, it is possible to use a C-mount lens with a CS-mount camera.

Mixing and Matching
C-mount and CS-mount components have identical threads, but lenses and cameras of different mount types should not be directly attached to one another. If this is done, the lens' focal plane will not coincide with the camera's sensor plane due to the difference in FFD, and the image will be blurry.

With an adapter, a C-mount lens can be used with a CS-mount camera (Figures 3 and 4). The adapter increases the separation between the lens and the camera's sensor by 5.0 mm, to ensure the lens' focal plane aligns with the camera's sensor plane.

In contrast, the shorter FFD of CS-mount lenses makes them incompatible for use with C-mount cameras (Figure 5). The lens and camera housings prevent the lens from mounting close enough to the camera sensor to provide an in-focus image, and no adapter can bring the lens closer.

It is critical to check the lens and camera parameters to determine whether the components are compatible, an adapter is required, or the components cannot be made compatible.

1.000"-32 Threads
Imperial threads are properly described by their diameter and the number of threads per inch (TPI). In the case of both these mounts, the thread diameter is 1.000" and the TPI is 32. Due to the prevalence of C-mount devices, the 1.000"-32 thread is sometimes referred to as a "C-mount thread." Using this term can cause confusion, since CS-mount devices have the same threads.

Measuring Flange Focal Distance
Measurements of flange focal distance are given for both lenses and cameras. In the case of lenses, the FFD is measured from the lens' flange surface (Figures 1 and 2) to its focal plane. The flange surface follows the lens' planar back face and intersects the base of the external 1.000"-32 threads. In cameras, the FFD is measured from the camera's front face to the sensor plane. When the lens is mounted on the camera without an adapter, the flange surfaces on the camera front face and lens back face are brought into contact.

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Figure 5: A CS-mount lens is not directly compatible with a C-mount camera, since the light focuses before the camera's sensor. Adapters are not useful, since the solution would require shrinking the flange focal distance of the camera (blue arrow).

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Figure 4: An adapter with the proper thickness moves the C-mount lens away from the CS-mount camera's sensor by an optimal amount, which is indicated by the length of the purple arrow. This allows the lens to focus light on the camera's sensor, despite the difference in FFD.

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Figure 3: A C-mount lens and a CS-mount camera are not directly compatible, since their flange focal distances, indicated by the blue and yellow arrows, respectively, are different. This arrangement will result in blurry images, since the light will not focus on the camera's sensor.

Date of Last Edit: July 21, 2020

Do Thorlabs' scientific cameras need an adapter?

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Figure 6: An adapter can be used to optimally position a C-mount lens on a camera whose flange focal distance is less than 17.526 mm. This sketch is based on a Zelux camera and its SM1A10Z adapter.

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Figure 7: An adapter can be used to optimally position a CS-mount lens on a camera whose flange focal distance is less than 12.526 mm. This sketch is based on a Zelux camera and its SM1A10 adapter.

All Kiralux™ and Quantalux^® scientific cameras are factory set to accept C-mount lenses. When the attached C-mount adapters are removed from the passively cooled cameras, the SM1 (1.035"-40) internal threads in their flanges can be used. The Zelux scientific cameras also have SM1 internal threads in their mounting flanges, as well as the option to use a C-mount or CS-mount adapter.

The SM1 threads integrated into the camera housings are intended to facilitate the use of lens assemblies created from Thorlabs components. Adapters can also be used to convert from the camera's C-mount configurations. When designing an application-specific lens assembly or considering the use of an adapter not specifically designed for the camera, it is important to ensure that the flange focal distances (FFD) of the camera and lens match, as well as that the camera's sensor size accommodates the desired field of view (FOV).

Made for Each Other: Cameras and Their Adapters
Fixed adapters are available to configure the Zelux cameras to meet C-mount and CS-mount standards (Figures 6 and 7). These adapters, as well as the adjustable C-mount adapters attached to the passively cooled Kiralux and Quantalux cameras, were designed specifically for use with their respective cameras.

While any adapter converting from SM1 to 1.000"-32 threads makes it possible to attach a C-mount or CS-mount lens to one of these cameras, not every thread adapter aligns the lens' focal plane with a specific camera's sensor plane. In some cases, no adapter can align these planes. For example, of these scientific cameras, only the Zelux can be configured for CS-mount lenses.

The position of the lens' focal plane is determined by a combination of the lens' FFD, which is measured in air, and any refractive elements between the lens and the camera's sensor. When light focused by the lens passes through a refractive element, instead of just travelling through air, the physical focal plane is shifted to longer distances by an amount that can be calculated. The adapter must add enough separation to compensate for both the camera's FFD, when it is too short, and the focal shift caused by any windows or filters inserted between the lens and sensor.

Flexiblity and Quick Fixes: Adjustable C-Mount Adapter
Passively cooled Kiralux and Quantalux cameras consist of a camera with SM1 internal threads, a window or filter covering the sensor and secured by a retaining ring, and an adjustable C-mount adapter.

A benefit of the adjustable C-mount adapter is that it can tune the spacing between the lens and camera over a 1.8 mm range, when the window / filter and retaining ring are in place. Changing the spacing can compensate for different effects that otherwise misalign the camera's sensor plane and the lens' focal plane. These effects include material expansion and contraction due to temperature changes, positioning errors from tolerance stacking, and focal shifts caused by a substitute window or filter with a different thickness or refractive index.

Adjusting the camera's adapter may be necessary to obtain sharp images of objects at infinity. When an object is at infinity, the incoming rays are parallel, and location of the focus defines the FFD of the lens. Since the actual FFDs of lenses and cameras may not match their intended FFDs, the focal plane for objects at infinity may be shifted from the sensor plane, resulting in a blurry image.

If it is impossible to get a sharp image of objects at infinity, despite tuning the lens focus, try adjusting the camera's adapter. This can compensate for shifts due to tolerance and environmental effects and bring the image into focus.

Date of Last Edit: Aug. 2, 2020

Why can the FFD be smaller than the distance separating the camera's flange and sensor?

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Figure 9: Refraction causes the ray's angle with the optical axis to be shallower in the medium than in air (θ_m vs. θ_o ), due to the differences in refractive indices (n_m vs. n_o ). After travelling a distance d in the medium, the ray is only h_m closer to the axis. Due to this, the ray intersects the axis Δf beyond the f point.;

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Figure 8: A ray travelling through air intersects the optical axis at point f. The ray is h_o closer to the axis after it travels across distance d. The refractive index of the air is n_o .

Equations for Calculating the Focal Shift (Δf )
Angle of Ray in Air, from Lens f-Number ( f / N )
Change in Distance to Axis, Travelling through Air (Figure 8)
Angle of Ray to Axis, in the Medium (Figure 9)
Change in Distance to Axis, Travelling through Optic (Figure 9)
Focal Shift Caused by Refraction through Medium (Figure 9)	Exact Calculation
	Paraxial Approximation

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Figure 11: Tolerance and / or temperature effects may result in the lens and camera having different FFDs. If the FFD of the lens is shorter, images of objects at infinity will be excluded from the focal range. Since the system cannot focus on them, they will be blurry.

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Figure 10: When their flange focal distances (FFD) are the same, the camera's sensor plane and the lens' focal plane are perfectly aligned. Images of objects at infinity coincide with one limit of the system's focal range.

Flange focal distance (FFD) values for cameras and lenses assume only air fills the space between the lens and the camera's sensor plane. If windows and / or filters are inserted between the lens and camera sensor, it may be necessary to increase the distance separating the camera's flange and sensor planes to a value beyond the specified FFD. A span equal to the FFD may be too short, because refraction through windows and filters bends the light's path and shifts the focal plane farther away.

If making changes to the optics between the lens and camera sensor, the resulting focal plane shift should be calculated to determine whether the separation between lens and camera should be adjusted to maintain good alignment. Note that good alignment is necessary for, but cannot guarantee, an in-focus image, since new optics may introduce aberrations and other effects resulting in unacceptable image quality.

A Case of the Bends: Focal Shift Due to Refraction
While travelling through a solid medium, a ray's path is straight (Figure 8). Its angle (θ_o ) with the optical axis is constant as it converges to the focal point (f ). Values of FFD are determined assuming this medium is air.

When an optic with plane-parallel sides and a higher refractive index (n_m ) is placed in the ray's path, refraction causes the ray to bend and take a shallower angle (θ_m ) through the optic. This angle can be determined from Snell's law, as described in the table and illustrated in Figure 9.

While travelling through the optic, the ray approaches the optical axis at a slower rate than a ray travelling the same distance in air. After exiting the optic, the ray's angle with the axis is again θ_o , the same as a ray that did not pass through the optic. However, the ray exits the optic farther away from the axis than if it had never passed through it. Since the ray refracted by the optic is farther away, it crosses the axis at a point shifted Δf beyond the other ray's crossing. Increasing the optic's thickness widens the separation between the two rays, which increases Δf.

To Infinity and Beyond
It is important to many applications that the camera system be capable of capturing high-quality images of objects at infinity. Rays from these objects are parallel and focused to a point closer to the lens than rays from closer objects (Figure 9). The FFDs of cameras and lenses are defined so the focal point of rays from infinitely distant objects will align with the camera's sensor plane. When a lens has an adjustable focal range, objects at infinity are in focus at one end of the range and closer objects are in focus at the other.

Different effects, including temperature changes and tolerance stacking, can result in the lens and / or camera not exactly meeting the FFD specification. When the lens' actual FFD is shorter than the camera's, the camera system can no longer obtain sharp images of objects at infinity (Figure 11). This offset can also result if an optic is removed from between the lens and camera sensor.

An approach some lenses use to compensate for this is to allow the user to vary the lens focus to points "beyond" infinity. This does not refer to a physical distance, it just allows the lens to push its focal plane farther away. Thorlabs' Kiralux™ and Quantalux^® cameras include adjustable C-mount adapters to allow the spacing to be tuned as needed.

If the lens' FFD is larger than the camera's, images of objects at infinity fall within the system's focal range, but some closer objects that should be within this range will be excluded. This situation can be caused by inserting optics between the lens and camera sensor. If objects at infinity can still be imaged, this can often be acceptable.

Not Just Theory: Camera Design Example
The C-mount, hermetically sealed, and TE-cooled Quantalux camera has a fixed 18.1 mm spacing between its flange surface and sensor plane. However, the FFD (f ) for C-mount camera systems is 17.526 mm. The camera's need for greater spacing becomes apparent when the focal shift due to the window soldered into the hermetic cover and the glass covering the sensor are taken into account. The results recorded in the table beneath Figure 9 show that both exact and paraxial equations return a required total spacing of 18.1 mm.

Date of Last Edit: July 31, 2020

当社ではZelux™、Kiralux^®、Quantalux^®ならびにサイエンティフィックCCDの4つのシリーズのサイエンティフィックカメラをご提供しております。Zeluxカメラは汎用的なイメージング向けで、設置面積が小さいながら高いイメージング性能を発揮します。Kiraluxカメラにはモノクロ、カラー、近赤外(NIR)強化型または偏光検出型のCMOSセンサーが搭載されています。コンパクトなパッシブ放熱型の筐体に納められているタイプのほか、カメラCC505MUのようにハーメチックシールされた熱電(TE)冷却型の筐体に納められたタイプもございます。偏光検出型Kiraluxカメラにはマイクロ偏光子アレイが組み込まれており、ThorCam™ソフトウェアパッケージを使用すると、直線偏光度、方位角、およびピクセルレベルでの強度を表す画像を取得することができます。QuantaluxモノクロsCMOSカメラは、低光量でも使用できるように広いダイナミックレンジと低い読み出しノイズという特徴を備えています。パッシブ冷却方式のコンパクトな筐体、またはハーメチックシールされたTE冷却素子付き筐体でご用意しています。当社のサイエンティフィックCCDカメラには、UV、可視、近赤外の各波長域用に最適化されたモデル、高フレームレートのカメラ、TE冷却素子付きまたは非冷却式の筐体、センサーフェイスプレートの無いモデルなど、様々な特徴を備えたモデルがございます。下の表では当社のカメラのラインナップの概要がご覧いただけます。

Compact Scientific Cameras
Camera Type	Zelux™ CMOS	Kiralux® CMOS					Quantalux® sCMOS
	1.6 MP	1.3 MP	2.3 MP	5 MP	8.9 MP	12.3 MP	2.1 MP
Item #	Monochrome: CS165MUa Color: CS165CUa	Mono.: CS135MU Color: CS135CU NIR-Enhanced Mono.: CS135MUN	Mono.: CS235MU Color: CS235CU	Mono., Passive Cooling: CS505MU Mono., Active Cooling: CC505MU Color: CS505CU Polarization: CS505MUP	Mono.: CS895MU Color: CS895CU	Mono.: CS126MU Color: CS126CU	Monochrome, Passive Cooling: CS2100M-USB Active Cooling: CC215MU
Product Photos (Click to Enlarge)
Electronic Shutter	Global Shutter	Global Shutter					Rolling Shutterb
Sensor Type	CMOS	CMOS					sCMOS
Number of Pixels (H x V)	1440 x 1080	1280 x 1024	1920 x 1200	2448 x 2048	4096 x 2160	4096 x 3000	1920 x 1080
Pixel Size	3.45 µm x 3.45 µm	4.8 µm x 4.8 µm	5.86 µm x 5.86 µm	3.45 µm x 3.45 µm			5.04 µm x 5.04 µm
Optical Format	1/2.9" (6.2 mm Diag.)	1/2" (7.76 mm Diag.)	1/1.2" (13.4 mm Diag.)	2/3" (11 mm Diag.)	1" (16 mm Diag.)	1.1" (17.5 mm Diag.)	2/3" (11 mm Diag.)
Peak Quantum Efficiency (Click for Plot)	Monochrome: 69% at 575 nm Color: Click for Plot	Monochrome: 59% at 550 nm Color: Click for Plot NIR: 60% at 600 nm	Monochrome: 78% at 500 nm Color: Click for Plot	Monochrome & Polarization: 72% (525 to 580 nm) Color: Click for Plot	Monochrome: 72% (525 to 580 nm) Color: Click for Plot	Monochrome: 72% (525 to 580 nm) Color: Click for Plot	Monochrome: 61% (at 600 nm)
Max Frame Rate (Full Sensor)	34.8 fps	92.3 fps	39.7 fps	35 fps	20.8 fps	14.6 fps	50 fps
Read Noise	< 4.0 e- RMS	< 7.0 e- RMS	< 7.0 e- RMS	< 2.5 e- RMS			< 1 e- Median RMS; <1.5 e="" span="">- RMS
Digital Output	10 Bit (Max)	10 Bit (Max)	12 Bit (Max)				16 Bit (Max)
PC Interface	USB 3.0
Available Fanless Cooling	N/A	N/A	N/A	0 °C at 20 °C Ambient (CC505MU Only)	N/A		0 °C at 20 °C Ambient (CC215MU Only)
Housing Size (Click for Details)	0.59" x 1.72" x 1.86" (15.0 x 43.7 x 47.2 mm3)	Passively Cooled CMOS Camera TE-Cooled CMOS Camera					Passively Cooled sCMOS Camera TE-Cooled sCMOS Camera
Typical Applications	General Purpose Imaging, Brightfield Microscopy, Machine Vision & Robotics, UAV, Drone, & Handheld Imaging, Inspection, Monitoring	VIS/NIR Imaging, Electrophysiology/Brain Slice Imaging, Materials Inspection, Multispectral Imaging, Ophthalmology/Retinal Imaging, Vascular Imaging, Laser Speckle Imaging, Semiconductor Inspection, Fluorescence Microscopy, Brightfield Microscopy	Fluorescence Microscopy, Immunohistochemistry, Machine Vision, Inspection, General Purpose Imaging	Mono. & Color: Fluorescence Microscopy, Immunohistochemistry, Machine Vision & Inspection Polarization: Machine Vision & Inspection, Transparent Material Detection, Surface Reflection Reduction	Fluorescence Microscopy, Immunohistochemistry, Large FOV Slide Imaging, Machine Vision, Inspection		Fluorescence Microscopy, VIS/NIR Imaging, Quantum Dots, Autofluorescence, Materials Inspection, Multispectral Imaging

• こちらの型番はZeluxシリーズ製品となります。これらのカメラには外部トリガ機能の有るタイプと、無いタイプがございます。
• このローリングシャッタには、照明が均一になるようにカメラと光源を同期させるEqual Exposure Pulse(EEP)モードが付いています。

Scientific CCD Cameras
Camera Type	Fast Frame Rate VGA CCD		1.4 MP CCD	4 MP CCD	8 MP CCD
Item # Prefix	Monochrome: 340M	UV-Enhanced Monochrome: 340UV	Monochrome: 1501M Color: 1501C	Monochrome: 4070M Color: 4070C	Monochrome: 8051M Color: 8051C	Monochrome, No Sensor Face Plate: S805MU
Product Photo (Click to Enlarge)
Electronic Shutter	Global Shutter
Sensor Type	CCD
Number of Pixels (H x V)	640 x 480		1392 x 1040	2048 x 2048	3296 x 2472
Pixel Size	7.4 µm x 7.4 µm		6.45 µm x 6.45 µm	7.4 µm x 7.4 µm	5.5 µm x 5.5 µm
Optical Format	1/3" (5.92 mm Diagonal)		2/3" (11 mm Diagonal)	4/3" (21.4 mm Diagonal)	4/3" (22 mm Diagonal)
Peak QE (Click for Plot)	55% at 500 nm	10% at 485 nm	Monochrome: 60% at 500 nm Color: Click for Plot	Monochrome: 52% at 500 nm Color: Click for Plot	Monochrome: 51% at 460 nm Color: Click for Plot	51% at 460 nm
Max Frame Rate (Full Sensor)	200.7 fps (at 40 MHz Dual-Tap Readout)		23 fps (at 40 MHz Single-Tap Readout)	25.8 fps (at 40 MHz Quad-Tap Readout)a	17.1 fps (at 40 MHz Quad-Tap Readout)b	17.1 fps (at 40 MHz Quad-Tap Readout)
Read Noise	< 15 e- at 20 MHz		< 7 e- at 20 MHz (Standard Models) < 6 e- at 20 MHz (-TE Models)	< 12 e- at 20 MHz	< 10 e- at 20 MHz
Digital Output (Max)	14 Bitc		14 Bit	14 Bitc		14 Bit
Available Fanless Cooling	Passive Thermal Management		-20 °C at 20 °C Ambient Temperature		-10 °C at 20 °C Ambient	Passive Thermal Management
Available PC Interfaces	USB 3.0 or Gigabit Ethernet					USB 3.0
Housing Dimensions (Click for Details)	Non-Cooled Scientific CCD Camera		Cooled Scientific CCD Camera Non-Cooled Scientific CCD Camera			No Face Plate Scientific CCD Camera
Typical Applications	Ca++ Ion Imaging, Particle Tracking, Flow Cytometry, SEM/EBSD, UV Inspection		Fluorescence Microscopy, VIS/NIR Imaging, Quantum Dots, Multispectral Imaging, Immunohistochemistry (IHC), Retinal Imaging	Fluorescence Microscopy, Transmitted Light Microscopy, Whole-Slide Microscopy, Electron Microscopy (TEM/SEM), Inspection, Material Sciences	Fluorescence Microscopy, Whole-Slide Microscopy, Large FOV Slide Imaging, Histopathology, Inspection, Multispectral Imaging, Immunohistochemistry (IHC)	Beam Profiling & Characterization, Interferometry, VCSEL Inspection, Quantitative Phase-Contrast Microscopy, Ptychography, Digital Holographic Microscopy

• 40 MHz、2タップ読み出しのギガビットイーサネットカメラの場合は最大13 fpsです。ギガビットイーサネットカメラでは4タップの読み出し機能はありません。
• 40 MHz、2タップ読み出しのギガビットイーサネットカメラの場合は最大8.5 fpsです。ギガビットイーサネットカメラでは4タップの読み出し機能はありません。
• 2タップ読み出しモードで動作するギガビットイーサネットカメラのデジタル出力は最大12ビットです。