Confocal Scanner System for Long- term Live Cell Imaging

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Hironori Takai1 Kenji Hachiya1 Youhei Kuwabara2 Takayuki Kei1

The CV1000 is a new confocal microscopy system that enables multi-point, long-term 3D imaging of live cells while keeping them healthy and active. Based on Yokogawa's CSU confocal scanner, the all-in-one CV1000 is equipped with laser light sources, highly sensitive EMCCD camera, precision XYZ auto stage, auto-focus and incubator functions. This system can be widely used by many researchers, especially for long-term observation of the development process of mammalian embryos, colony formation process of iPS/ES cells, and so on.

  1. Development Dept., Life Science Headquarters
  2. Sales Dept., Life Science Headquarters

INTRODUCTION

As fluorescent proteins including green fluorescent protein (GFP) have been put into practice, biotechnology research that employs imaging that uses them has progressed greatly. In particular, observation with a confocal system has become popular for its clear images, yielding many successful results1,2. Yokogawa's CSU series confocal scanners3 have been widely used as fluorescent protein gains popularity and are now well-recognized as a useful tool for observing live cells.

The major reason why the CSU series has gained popularity in the market is its high-speed processing capability and low phototoxicity to cells. Combining these optical technologies in the CSU series with Yokogawa's excellent environmental control and precise positioning technologies, the Life Science Headquarters has developed the CellVoyager CV1000 confocal scanner system to observe live cells. This product can be used not only for biological basic research but also for research in new drug development and regenerative medicine. We aim to make this product a de facto standard tool in biotechnology.

The CV1000 satisfies all the following requirements for observing live cells.

  • Extremely low phototoxicity to cells
  • High-speed processing to track the behavior of live cells
  • Accuracy and high reproducibility
  • Robustness and reliability for long-term usage
  • Easy-to-use software

The main specifications of the unit are as follows:

  • Excitation light source: Three-color laser (405 nm, 488 nm, and 561 nm), LED transmission for the bright field
  • Confocal unit: Pinhole disk with microlens ( φ 25 μm and φ 50 μm)
  • Objective lens: Max. 6 lenses (4×, 10×, 20×, 40×, 60×, and 100×)
  • Auto-focus: By laser
  • Fluorescent filter wheel: 6 positions
  • Camera: Back-illuminated EMCCD camera
  • Temperature control unit: 30°C to 40°C (normal temperature), 17°C to 30°C (low temperature)
  • CO2 concentration control unit: 5%
  • Humidity control: Forced humidification
  • Control software This paper outlines the CV1000 and describes characteristics of its hardware and software.

OUTLINE AND CONFIGURATION OF CV1000

Figure-1-External-view-of-the-CV1000 
Figure 1 External view of the CV1000

Figure 1 shows the external view of the CV1000, consisting of the main body, power supply unit, and PC for control. The main body consists of three parts: the environmental control system for culturing cells; the optical system for a confocal microscope; and the mechatronic part including the XY stage for conveying specimens and the Z stage for adjusting the objective lens position. The CV1000 supports various culturing containers such as slide glasses, cover glass chambers, glass bottom dishes, and micro plates.

The CV1000 is a compact all-in-one system. The observation part is completely shielded from outside light, requiring no dark room facility. Media for cell cultures can be exchanged without opening the cover. The CV1000 can keep a stable environment to perform experiments for up to one week.

Conventional confocal microscopes require much effort and know-how for everything from installation to operation, which depends on a user's skills. The CV1000 is a turn-key system which requires no operational expertise in hardware and software for operation, and can be used in various researches.

Software

 Figure-2-A-screen-of-the-CV1000-control-software
Figure 2 A screen of the CV1000 control software

Figure 2 shows a screen of the CV1000 control software for capturing images and controlling equipment. This screen is designed so that users do not need to pay attention to hardware. Users can quickly obtain images by clicking a single button even with a default configuration.

The control software has various features for setting experimental conditions and imaging procedures, editing obtained images, creating movies and the like. Even during imaging, users can easily select a specimen from a preview map, obtain the whole view of a specimen in culturing containers such as dishes, select and observe multipoint images, and check obtained images.

Thanks to the high-speed, high-precision XYZ stage, imaging can be performed quite smoothly while changing observation views and selecting the position in depth direction.

The platform is Microsoft Windows 7 64-bit version with .NET 4.0 Framework. On a 64-bit operating system, the software can use more than 2 GB memory to easily process a 2 MB three-dimensional stack image output from a 1-megapixel 16-bit color camera.

Figure-3-The-outline-of-the-MVVM-pattern 
Figure 3 The outline of the MVVM pattern

Technologies such as the C# 3.0, Windows Presentation Foundation (WPF), and Shader Effect are used. Language Integrated Query (LINQ) in C# 3.0 helps the software to be written in declare statements, making it less complex. WPF is used as a GUI platform to enhance GUI expression and flexibility. The Shader Effect is used for image processing calculation. It enables high-speed calculation with a graphic card to process images obtained at four different wavelengths and display their merged image.

For the software architecture, we use the Model View ViewModel (MVVM) pattern as shown in Figure 3. By using data binding functions in WPF, we have developed the software with sophisticated GUI while keeping loose the coupling between GUI and logic.

This architecture helps ensure easy maintenance of software and improve the design quality.

The optical system for the confocal microscope

 Figure-4-The-optical-system-of-the-CV1000
Figure 4 The optical system of the CV1000

Figure 4 shows the optical system of the CV1000. As an excitation light source, lasers with three wavelengths (405 nm, 488 nm, and 561 nm) are provided to support popular fluorescent dye and fluorescent proteins such as Hoechst, DAPI, GFP, and mREP. These three laser beams are multiplexed, paralleled through the collimate lens, and enter the confocal scanner. Through the microlens array, these parallel lights become multiple point lights, and then each point light passes through the corresponding pinhole. Then, the point lights pass through the tube lens and objective lens and focus on the specimen to excite cells. When fluorescence is excited from a fluorescent-labeled target in the specimen, the fluorescence passes through the objective lens and tube lens in the opposite direction of the excitation light and enters the confocal scanner. After passing through the pinhole array, the fluorescence signals form a confocal image, which is reflected by the dichroic mirror (DM), passes through the relay lens, and forms an image on the camera.

Different fluorescent-labeled proteins are used for respective observation targets. Exciting lights with wavelengths corresponding to respective fluorescents are selectively turned on and off, and at the same time, the fluorescent filter in front of the camera is switched, and then pictures are sequentially taken for each wavelength. Finally, those single-color images are superimposed to create a multicolor image.

To observe the three-dimensional structure of cells, the Z stage is used to move the objective lens along the light axis, and cross-sectional images of cells are obtained for each submicron-to-few-micron movement. Then, those images are stacked to create a three-dimensional image.

To observe the appearance of cells, LED transmission is used for a bright field light source.

To support various observations from a wide view to small targets such as endoplasmic reticulum in cells, this system has six objective lenses ranging from 4× to 100×, which can be electrically switched.

The confocal scanner with selectable pinhole size

The major advantage of confocal systems is higher resolution in the Z-direction (the direction of depth of the specimen) than that of epi-fluorescence systems. The higher resolution in the Z-direction helps obtain thinner optical slices and thus the fine structure of cells can be observed. The thickness of the optical slice is determined by the following equation (1) with variables such as the pinhole diameter, numerical aperture (NA) of objective lens, and wavelength of fluorescence4. This equation clearly shows that a thinner optical slice can be obtained by an objective lens with a larger NA and pinholes with a smaller diameter.

Equation-Confocal-Scanner-System

Figure-5-The-relationship-between-pinhole-diameter-and 
Figure 5 The relationship between pinhole
diameter and optical slice thickness (λ: 520 nm)

Where:
λem: Fluorescence wavelength
n: Refractive index of medium between the objective lens and the specimen container
NA: Numerical aperture of the objective lens
PH: Pinhole diameter

Figure 5 shows the thickness of an optical slice obtained by the equation (1) by substituting the wavelength of GFP (520 nm) for l em and numerical apertures of typical objective lens for NA. The lower the magnification the objective lens has and the smaller the diameter the pinhole has, the thinner an optical slice can be obtained. In other words, larger confocal effects are very effective.

 Figure-6-The-point-spread-function-PSF-of-the-CV1000
Figure 6 The point spread function (PSF)
of the CV1000

Based on the results shown in Figure 5, Yokogawa's CSU confocal scanners use objective lenses with high magnification alone. The diameter of pinholes is set to 50 μm; due to a limitation to the structure of scanners, it is difficult to change this value. When a lens with low magnification is used for morphological observation, the confocal system does not exert its full effects. Therefore, confocal scanners are mainly used for research that needs high magnification. To overcome the limitation, the CV1000 has two disks with pinholes of 50 μm and 25 μm respectively to satisfy a strong demand for diameter selectivity. Overcoming the disadvantage of the conventional CSU, a single CV1000 exerts full confocal effect with various objective lenses from low to high magnification.

Figure 6 shows the actual measurement result of the point spread function for different pinhole diameters when the objective lens (10×, NA = 0.4) is used. The point image of the 25 μm pinhole is about 15% narrower than that of 50 μm, showing the superiority of small pinholes. In addition, smaller pinholes reduce crosstalk caused by lights from other than the focal plane and improve the S/N ratio of confocal images.

Figure 7 shows sample images of cells. The Z-section image of φ 25 μm pinholes is sharper than that of φ 50 μm pinholes.

High-precision environmental control

In the developmental process research, samples such as fertilized eggs and early embryos are incubated and observed over a dozen days. Since these samples are sensitive to the ambient environment, the success of the experiment depends heavily on the environmental control.

Figure-7-Sample-images-of-cells 
Figure 7 Sample images of cells (10×, NA = 0.4)

For the CV1000, a highly stable environmental chamber has been developed to keep the temperatures between 30°C and 40°C, humidity at 90% or more, and CO2 concentration at 5% in the measurement part. For example, a chamber for a single dish can keep the temperature in the above-mentioned range with a fluctuation of ± 0.1°C. To ensure this performance, we have made various improvements. Specifically, the housing is covered with a thick heat insulator to reduce the impact from the outside temperature fluctuation, making the inside environment similar to that in a thermostatic chamber. Furthermore, to curb temperature fluctuation in the chamber, the chamber is divided into several zones from top to bottom and respective temperatures are independently controlled by heaters and temperature sensors mounted in each zone. The temperature of the objective lenses is also controlled individually to eliminate even a slight temperature change during replacement.

Figure 8 shows an example of temperature control. After the transition period, the fluctuation of the temperature in the chamber is controlled to within ± 0.1°C, which ensures the high temperature stability in the observation part.

Figure 9 shows an example of CO2 concentration control in the chamber. When culturing cells, the ambient CO2 concentration is usually controlled at 5% to keep the pH value of the medium constant. 100% CO2 is mixed with air and the concentration is controlled by using a near-infrared gas sensor. The concentration becomes stable about five minutes after the start of control.

 Figure-8-Example-of-temperature-control Figure-9-Example-of-the-CO-2-concentration-contro 
Figure 8 Example of temperature control Figure 9 Example of the CO2 concentration control

CONCLUSION

Bio-imaging technologies for visualizing minute behavior in cells have contributed a lot to clarifying life phenomena. The need for higher-speed, more precise, and longer-term observation of behavior of proteins in live cells is sure to increase. Yokogawa will respond to this need and offer ideal devices for research.

REFERENCES

  1. K. Matsuura-Tokita, M. Takeuchi, et al., "Live imaging of yeast Golgi cisternal maturation," Nature, Vol. 441, No. 7096, 2006, pp. 1007- 1010
  2. K. Yamagata, R. Suetsugu, et al., "Long-term, six-dimensional live- cell imaging for the mouse preimplantation embryo that does not affect full-term development," J Reprod Dev, Vol. 55, No. 3, 2009, pp. 343-350
  3. Hideo Hirukawa, Hiroshi Nakayama, et al., "New Technologies for CSU-X1 Confocal Scanner Unit," Yokogawa Technical Report English Edition, No. 45, 2008, pp. 21-26
  4. S. Wilhelm, B. Grobler, M. Gluch, H. Heinz, "Confocal Laser Scanning Microscopy : Optical Image Formation and Electronic Signal Processing," Carl Zeiss Jena GmbH, 45-0029 e/09.03, pp. 15
  • CSU is a registered trademark of Yokogawa Electric Corporation.
  • Cell Voyager is a registered trademark of Yokogawa Electric Corporation.
  • CV1000 is a registered trademark of Yokogawa Electric Corporation.

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