Confocal microscopy
Why use a confocal
microscope?
Confocal microscopy offers several advantages over conventional optical microscopy including;
i.
Increased
effective resolution: Confocal microscopy produces images of improved
resolution, up to 1.4 times greater than standard microscopy and also has a
higher level of sensitivity compared to conventional microscopes, due to highly
sensitive light detectors and the ability to accumulate images captured over
time.
ii.
Clear
examination of thick specimens (Controllable depth of field): Double and
triple labels can be collected with a confocal microscope. Since these images
are collected from an optical plane within the sample, precise colocalizations
can be performed.
iii. Reduced blurring of image from light scattering: Eliminates the out of focus "haze" normally seen with a fluorescent sample. Fine detail is often obscured by the haze and cannot be detected in a non-confocal, fluorescent microscope.
iv. Improved signal to noise ratio
v. Z-axis scanning: The confocal microscope has a stepper motor attached to the fine focus, enabling the collection of a series of images through a three dimensional object. These images can then be used for a two or three dimensional reconstruction.
vi. Magnification can be adjusted electronically
Purpose (Applications):
Confocal microscopy is used in a large variety of scientific fields.
i. Esterase activity
ii. Oxidation reaction
iii. Intracellular pH
iv. Intracellular Calcium
v. Phagocytosis and Internalization
vi. Apoptosis
vii. Membrane potential
viii. Cell-cell communication (Gap junction)
How does a confocal microscope work?
Confocal microscopy generally uses a monochromatic light source (usually a laser) to excite fluorescent dyes. The light source is then focused into a single plane or spot which can be scanned across the specimen on one focal plane at a time. The thickness of the spot or plane of light is usually between 0.25 and 2 mm. The light is then scanned across the specimen by an oscillating mirror. In essence the confocal microscope optically sections the specimen. The specimen can then be raised and lowered so that the light can slice through at different planes. This process eliminates the problem of out of focus fluorescence. Subsequently, images from different focal planes can be digitized and overlayed to produce a single composite image with superior contrast or the images can be stacked and stored digitally as a three dimensional image.
A laser is used to provide the
excitation light (in order to get very high intensities). The laser light
(blue) reflects off a dichroic mirror. From there, the laser hits two mirrors
which are mounted on motors; these mirrors scan the laser across the sample.
Dye in the sample fluoresces, and the emitted light (green) gets descanned by
the same mirrors that are used to scan the excitation light (blue) from the
laser. The emitted light passes through the dichroic and is focused onto the
pinhole. The light that passes through the pinhole is measured by a detector,
i.e., a photomultiplier tube (PMT).
Glossary and techniques:
Laser Systems:
The lasers commonly employed in laser
scanning confocal microscopy are high-intensity monochromatic light sources.
Pinhole: In confocal microscopy, variable diaphragm pinhole
apertures placed near the light source and detector enable the microscope to
produce thin optical sections of focal planes in the specimen. A pinhole refers
to a small break in the coating (primarily arising in the thin-films of
interference filters) produced by dust particles or debris on the substrate
during application. Pinhole size is measured against a standard under specific
conditions using a high-intensity illumination.
Photomultiplier
tube (PMT): An electrical device designed to collect and amplify photon
signals. Incoming photons strike a target in the face of the photomultiplier to
liberate free electrons, which are accelerated onto a dynode that in turn
liberates an amplified stream of electrons. Several dynodes are arranged in
series to produce a tremendous degree of amplification from each original
photon and then transmit the signal to a processing circuit. Unlike area-array
detectors such as charge-coupled devices (CCDs), photomultipliers do not
form an image.
Bleed-through
(Cross-over): Bleed-through of fluorescence emission, due to the broad
spectral profiles exhibited by common fluorophores, is a fundamental problem
that must be addressed in laser scanning confocal fluorescence microscopy. The
phenomenon is most often manifested by the emission of one fluorophore being
detected in the channel or through the filter combination reserved for a second
fluorophore.
Bleed-through occurs when unwanted wavelengths
are transmitted through an optical filter designed to block them. The effect
usually occurs when the design of a filter does not allow complete destructive
interference of wavelengths excluded from the bandpass region. Bleed-through is
also a problem when the incident light angle is highly oblique with respect to
the filter surface, or when the excitation and emission spectra of fluorescent
dyes overlap.
z-series and 3D image:
A popular mode of optical microscopy in which a focused laser beam is scanned laterally along the x and y axes of a specimen in a raster pattern. The emitted fluorescence (reflected light signal) is sensed by a photomultiplier tube (PMT) and displayed in pixels on a computer monitor. The pixel display dimensions are determined by the sampling rate of the electronics and the dimensions of the raster. Signal photons that are emitted away from the focal plane are blocked by a pinhole aperture located in a plane confocal with the specimen. This technique enables the specimen to be optically sectioned along the z axis.
A 3D image created by adding together multiple optical sections acquired along the z-axis of a confocal microscope. In conventional widefield fluorescence microscopy, images of three-dimensional specimens are often blurred due to emission occurring away from the immediate focal plane. The same images are often remarkably sharp when gathered with a confocal microscope.
Scanning modes:
Among the common scanning modes are point, line, free line, parallel plane, and rectangle scanning over one or more dimensions. Line scanning along the x, y, or z axis, or diagonally between axes, provides intensity information across a single set of coordinates in the lateral or axial dimension. This scanning mode is useful for obtaining accurate quantitative information about rapid physiological events, such as calcium waves or sparks.
Sequential scan mode:
In
sequential scan mode, images will be recorded in a sequential order instead of
acquiring them simultaneously in different channels. Each sequence can be
recorded using an individual set of user-defined parameters to optimize
performance and image quality. e.g. simultaneous image acquisition of double or
triple-stained samples can result in crosstalk since all dyes will be excited
at the same time. Defining parameter sets specific for each dye and executing
them in a sequential order can eliminate this crosstalk
Procedure (That I
follow in my lab. for capturing confocal image)
I infect the mice [Wild type (C57BL/6) vs CXCL10 knock out mice] with
1000 pfu/ml HSV-1 (3 µl) per eye. At different times post infection at day 3, 5
and 7, I euthanize the mice and harvest the cornea for detecting infiltrating CD4
and CD8 T cells (and also for colocalization of CXCL10 and virus antigen) using
Confocal microscopy.
A. Preparation of
Corneal mounts:
Fixation:
Blocking:
Staining:
Fixation:
DAPI:
B. Using confocal
microscopy (FV500):
- Click on “Dye”: Select dyes
(DAPI, FITC, TRITC or Alexa-633)
- Apply
- Click on Laser for chosen dyes:
Apply
-
Focus: X2, X4
-
-
Size: 512X512; high resolution 1024X1024
-
Mode:
(Generally, I use Kalman for sequential scan; select frame Kalman and
select 2 or 3)
- Mode: Sequential scan 123
Focus your slide and select only one laser at a time and detect the bleed through for that laser. If you detect bleed through, then follow the following instructions;
A. Select one laser, turn off others
Press Focus, Press Stop
i. Select channel 1 (DAPI), Select DAPI laser
ii. Press coloring tool
iii. Select following intensity mapping;
Gamma 1.0
Press Hi-Low High (red) ---------- Low (black or blue)
Adjust PMT, Gain and Offset
Press Focus, press Stop scan
B. Likewise select channel 2 and channel 3:
Click coloring tool (LUT), click Hi-Low and set up PMT, Gain, and Offset, select Gamma 1.0
C. After adjusting bleed-through, set coloring tool as according to dye color e.g. Blue for DAPI, Green for FITC and Red for TRITC. Apply.
7. Perform sequential scan selecting all dyes, lasers and selecting all required parameters.
8. After scanning, make 3D image using software. Analyze the observation.