HO-DHM-UT01 is a transmission type upright digital holography microscopes with balanced afocal configuration that uses infinity corrected plan achromatic objectives in both reference and object beams. A common tube lens is provided for achieving afocal imaging configuration with minimal aberrations. Sony make CMOS sensor is used for the recording of holographic images. A linearly polarized 650nm diode laser is used for illumination in the DHM system. A high bright LED illuminated brightfield observation with binocular viewing is also integrated in the system. Since users may not be familiar with phase images, the LED illumination can be used first to focus the cell sample as desired, followed by recording of the phase image using laser illumination.
In addition to the object beam objective, two low power objectives are also provided for larger FOV in brightfield observations. The nosepiece has a triple turret mechanism for holding three microscope objectives. The user can easily switch the objectives manually. As the low power objectives have large FOV, the user can use them first to locate the desired area of sample. A manually operated XY sample stage is provided for scanning the sample area. Once the sample area is located, the user can change the low power objective to high power objective for the magnified image of selected area.
A manually operated shutter with source selector switch is provided near the eyepiece for the safety of eyes by blocking the laser light to the eyepiece.
Once the desired area for phase imaging is selected in brighfield mode, the user can close the manual shutter and the system will be ready for QPI.
A complete user friendly software (Digital HM_V01) with laptop is provided with system for the recording and reconstruction of the images. The software uses patented unique single shot high resolution method for the phase image reconstruction.
Digital holographic microscope with user specified high end microscope objectives (Plan apochromatic, Plan fluorite, Extra-long WD etc.) may also be made available upon special requests.
Digital holographic microscopy is an emerging modality that offers capability of quantitative phase imaging (QPI) of transparent unstained cells in their most natural state. While phasesensitive imaging methodologies such as dark-field, phase contrast and differential interference contrast are known for several decades, they cannot provide quantitative phase information. DHM can achieve this by use of interferometric imaging concept. A schematic DHM system is shown in Fig. 1:
Fig.1: Schematic of a balanced DHM system that works on the interferometric imaging principle. The phase image is obtained by digital processing of the interference signal recorded using an array sensor.
SF : Spatial filter, BS : Beamsplitter, O : Object beam, R : Reference beam, MO1 / MO2 : Microscope Objectives
When a collimated laser beam passes through a transparent cell sample, typically very little light is absorbed. The laser wavefront however gets distorted due to the phase delay seen by the beam at each (x, y) location (see Fig. 2). The phase Φ (x, y) of the beam after passing through the sample may be described as:
Φ (x,y) = ( 2π / λ ) ∫ dz n (x, y, z)
Here λ is the wavelength of laser used and n (x, y, z) stands for the relative refractive index of the cell at location (x, y, z) relative to the surrounding medium. Clearly a strong phase signal is detected if there is large index difference between the cell and the surrounding medium. If the index of the cell is uniform over a region, the phase function can be approximately associated with the height map profile of the cell, thus giving a 3D perspective of the cell. Instead of employing external contrast agents, the DHM thus uses the natural refractive index contrast of the cells for imaging purpose. Refractive index is a property related to chemical composition and therefore a sensitive phase imaging system can have several applications in basic Bio-sciences and diagnostics.
Fig.2: Illustration of phase delay of a collimated laser beam wavefront as it passes through a transparent cell sample. The phase delay is due to differential optical path difference through different parts of the cell sample.
The Fourier Transform Method is a popular choice for processing of single shot interferometric imaging data. However this method is known to have poor spatial resolution which is well below the diffraction-limited resolution that the microscopic system can achieve. The IIT Delhi technology used in this product uses a novel constrained optimization approach to recovery of full-resolution phase images as illustrated in where bright-field and phase images of a cervical Fig. 3 cell are shown.
Fig.3: Illustration of phase images of red blood cells and patient cervical cells using Digital Holographic Microscopy system (a) Brightfield images, (b) phase images reconstructed using the traditional Fourier transform method, (c) high resolution phase images obtained using novel single shot phase imaging technology developed at IIT Delhi. The color coding in (b) and (c) indicates the phase map (approximately height map) of the cell.
|DHM type||:||Transmission, Upright|
|DHM configuration||:||Balanced, afocal|
|Measurement mode||:||Single wavelength|
|Source wavelength||:||650 nm|
|Source power||:||5 mW|
|Object beam microscope objective||:||Plan Achromatic (40X, 0.65 NA)|
|Reference beam microscope objective||:||Plan Achromatic (40X, 0.65NA)|
|Axial depth profiling accuracy||:||≤ 50 nm|
|Lateral resolution||:||≤ 1 μm|
|Camera Field of view||:||0.185 x 0.124 mm2|
|Sensor type||:||CMOS Color|
|Pixel class||:||6 MP|
|Resolution||:||3088 x 2076 Pixels|
|Aspect ratio||:||3 : 2|
|Pixel size||:||2.4 μm|
|Optical size||:||7.41 mm x 4.98mm|
|Gain (master / RGB)||:||14.5x / 5x|
|Pixel clock range||:||20 MHz - 474 MHz|
|Frame rate free run mode||:||58.0 fps|
|Frame rate trigger (continuous)||:||29.0 fps|
|Frame rate trigger (maximum)||:||29.0 fps|
|Exposure time (min – max)||:||0.013 ms – 999 ms|
|Long exposure (maximum)||:||120000 ms|
|Interface connector||:||USB 3.0|
|Phase image reconstruction||:||Patented single shot high resolution method|
|Optical system||:||Infinity corrected (200 mm tube lens)|
|Illumination system||:||High bright white LED, Intensity adjustable|
|Nosepiece||:||Triple, Rotating turret|
|Microscope Objectives||:||1. Plan Achromatic 10X, NA 0.25, 2mm FOV|
|2. Plan Achromatic 20X, NA 0.40, 1mm FOV|
|3. Plan Achromatic 40X, NA 0.65, 0.5mm FOV|
|Viewing head||:||Sidentopf Binocular head, 30o inclination, 48 -75mm IP adjustment|
|Eyepiece||:||10X wide field (FN20), diopter adjustable, High eye relief|
|Focusing||:||Coaxial coarse / fine focusing, fine 0.2mm / rotation|
|Sample Stage||:||Rectangular stage with specimen holder, XY travel - 78 x 54mm|
|Sample Stage drive||:||Manual, coaxial drop down knob|