Nanolive Imaging

The secrets behind Nanolive’s imaging patented technology

Nanolive’s 3D Cell Explorer’s technology is unique worldwide and is based on a fundamental patent (US 8,937,722 & EU WO 2011/121523).

The combination of holography and rotational scanning makes Nanolive imaging a revolutionary technology.

Holography offers a unique means to measure cells in their native environment: label-free, non-invasive, manipulation-free, and interference-free. Rotational scanning allows 3D reconstructions, noise robustness, and a resolution far beyond the accepted limit for light.

To achieve optimal results for every measurement, the optics of our technology are completely self-adjusting. It guarantees the best alignment conditions – whatever the environment is.

How does the 3D Cell Explorer produce cell images with better than 200 nm lateral resolution?

Classical Microscopy (e.g. fluorescence imaging)

The cell is directly imaged; so what you see on your camera is the image of the cell. Therefore, one absolutely needs to apply Nyquist sampling on the camera. But, this is NOT true for the 3D Cell Explorer. The paradigm shift to make is that there is no direct imaging of the cell on the camera.

Nanolive Imaging

Non-invasive optical nanoscopy can achieve such a lateral resolution by using a quasi-2π-holographic detection scheme and complex deconvolution. The spatial frequencies of the imaged cell do not make any sense to the human eye. But these SCATTERED frequencies are converted into a hologram and synthesize a bandpass which has a resolution DOUBLE the one normally available. Holograms are recorded from different illumination directions on the sample plane and observe sub-wavelength tomographic variations of the specimen. Nanoscale apertures serve to calibrate the tomographic reconstruction and to characterize the imaging system by means of the coherent transfer function. This gives rise to realistic inverse filtering and guarantees true complex field reconstruction.

All the math and proofs are explained in great detail in our peer reviewed Nature Photonics publication here:

Explaining the Resolution Jump

Rayleigh resolution for incoherent light (e.g. fluo) is 400nm=0.61*520nm/(0.8), for coherent light (e.g. holography) 533nm=0.82*520nm/(0.8) with the diffraction limit (e.g. any imaging by niquist) of 325nm=0.5*520nm/(0.8). In our case for the 3D Cell Explorer configuration, the maximal expected resolution is around 160nm=0.5*520nm/(2*0.8) and we estimate the real resolution (according to Rayleigh) to be about ~190nm. Therefore, taking into account the illuminating wavelength the experimental resolution is 190nm=/lambda/(3.5 NA), indicating a sub-diffraction resolution (d=325 nm at given wavelength and NA) imaging in far-field (non-fluorescent) transmission microscopy.

In conclusion, the 2 terminologies of (i) optical resolution (the real one) and (ii) sampling resolution (the one on the screen) are separated for 3D holotomographic microscopy. For the sake of computational cost-reduction, Nanolive chose to have the sampling optimal at the optical resolution, hence about 180 nm. Again, we can do this, thanks to our technology WITHOUT loosing any real resolution, but of course a user could over-sample the images and have double/triple/etc sampling on the screen with the same optical resolution (e.g. simple zero-padding in fft space to have a smoother image).

The images

We have chosen Mitochondria as a great candidate to demonstrate resolution. Below is an image calculating the separation between Mitochondria using standard signal profiling. In the example we resolve mitochondria tubules as thin as 186 nm (using full width at half maximum standard measurement of object thickness).

History of Microscopy

Technical Comparison

Please scroll the table right to see the full comparison

Properties nanolive signet Standard Fluorescence Super resolution Fluorescence Phase imaging Electrical impedance SEM, AFM
Time time_secs time_hour time_hour time_secs time_secs time_days
Simplicity green line simplicity2_small simplicity2_small green line simplicity2_small simplicity3_small
Cost green_money_icon Icons_50px_02-03 Icons_50px_02-03 green_money_icon Icons_50px_02-03 Icons_50px_02-02
Cell condition happy_face Icons_50px_02-07 Icons_50px_02-07 happy_face happy_face Icons_50px_02-06
Temporal sampling time_secs time_min time_min time_secs time_secs time_min
Live Cell Imaging checkmark_green Icons_50px_03-07 Icons_50px_03-07 checkmark_green checkmark_green Icons_50px_03-07
Training-free checkmark_green Icons_50px_03-07 Icons_50px_03-07 Icons_50px_03-03 Icons_50px_03-03 Icons_50px_03-07
Cellular health happy_face Icons_50px_02-07 Icons_50px_02-07 happy_face happy_face Icons_50px_02-06
 Lateral Resolution Below 200nm Down to 250nm Down to 50nm 400 – 1000nm No Image  5-10nm
Image Dimensionality 3d_cube_green Icons_50px_04-03 3d_cube_green Icons_50px_03-06 Icons_50px_04-02 3d_cube_green
Quantitative checkmark_green Icons_50px_03-07 Icons_50px_03-07 Icons_50px_03-03 checkmark_green Icons_50px_03-03
Comprehensive green_head_idea Icons_50px_04-04 Icons_50px_04-04 Icons_50px_04-04 Icons_50px_04-04 green_head_idea
Price (euro) euro_green Icons_50px_02-03 Icons_50px_02-04 euro_green Icons_50px_02-04

Marker-Free Imaging

Comparison with phase imaging

Traditional phase microscopy

Topography of Projected Cell

2D refractive index map


Tomography of cell

 2D section of the 2D RI map

Example of Embryonic Stem Cells (ESC) during mitosis



2D RI map of mouse Embryonic Stem Cell Cells (mESC)

Topography based on OPD

Cell projection (outside cell topography)

Total Optical Cell Density (2.5D OCD)

Resolution: 400 – 1000 nm

High noise level

Tomography Digital stains based on RI

Tomographic Imaging

Physical cell’s height (3D RI distribution)

200 nm resolution

Low noise ratio

Comparison between ESCs (4 & 5) as observed with the two technologies