Mechanical stability of a microscope setup working at a few kelvins for single-molecule localization

Superfluid helium nanoscope insert with millimeter working range

A superfluid helium insert was developed for cryogenic microscopy of millimeter-sized specimens. An optical-interferometric position sensor, cryogenic objective mirror, and piezo-driven cryogenic stage were fixed to an insert holder that was immersed in superfluid helium. The single-component design stabilized the three-dimensional position of the sample, with root-mean-square deviations of (x, lateral) 0.33 nm, (y, lateral) 0.29 nm, and (z, axial) 0.25 nm. Because of the millimeter working range of the optical sensor, the working range of the sample under the active stabilization was (x, y) 5 mm and (z) 3 mm in superfluid helium at 1.8 K. The insert was used to obtain the millimeter-sized fluorescence image of cell nuclei at 1.8 K without a sample exchange.

Cryogenic Far-Field Fluorescence Nanoscopy: Evaluation with DNA Origami

Far-field fluorescence localization nanoscopy of individual fluorophores at a temperature of 1.8 K was demonstrated using DNA origami as a one-nanometer-accurate scaffold. Red and near-infrared fluorophores were modified to the scaffold, and the fluorophores were 11 or 77 nm apart. We performed the localization nanoscopy of these two fluorophores at 1.8 K with a far-field fluorescence microscope. Under the cryogenic conditions, the fluorophores were perfectly immobilized and their photobleaching was drastically suppressed; consequently, the lateral spatial precision (a measure of reproducibility) was increased to 1 nm. However, the lateral spatial accuracy (a measure of trueness) remained tens of nanometers. We observed that the fluorophore centroids were laterally shifted as a function of the axial position. Because the orientation of the transition dipole of the fluorophores was fixed under cryogenic conditions, the anisotropic emission from the single fixed dipole had led to the lateral shift. This systematic error due to the dipole-orientation effect could be corrected by the three-dimensional localization of the individual fluorophores with spatial precisions of (lateral) 1 nm and (axial) 17 nm. In addition, the xy-error arising from the three-dimensional (3D) orientation of the scaffold with the two fluorophores 11 nm apart was estimated to be 0.3 nm. As a result, the individual fluorophores on the DNA origami were localized at the designed position, and the lateral spatial accuracy was quantified to be 4 nm in the standard error.

Nanometer Accuracy in Cryogenic Far-Field Localization Microscopy of Individual Molecules

We demonstrate the nanometer accuracy of far-field fluorescence localization microscopy at a temperature of 1.8 K using near-infrared and red fluorophores bonded to double-stranded DNA molecules (10.2 nm length). Although each fluorophore was localized with a 1 nm lateral precision by acquiring an image at one axial position within the focal depth of ±0.7 μm, the distance between the two fluorophores on the lateral plane (D_xy) was distributed from 0 to 50 nm. This systematic error was mainly due to detecting with the large focal depth the dipole emission from orientationally fixed fluorophores. Each fluorophore was localized with precisions of ±1 nm (lateral) and simultaneously ±11 nm (axial) by acquiring images every 100 nm in the axial direction from -900 to 900 nm. By correcting the dipole orientation effects, the distribution of D_xy was centered around the DNA length. The average and standard deviation of D_xy were 10 and 5 nm.

Three-Dimensional Localization of an Individual Fluorescent Molecule with Angstrom Precision

Among imaging techniques, fluorescence microscopy is a unique method to noninvasively image individual molecules in whole cells. If the three-dimensional spatial precision is improved to the angstrom level, various molecular arrangements in the cell can be visualized on an individual basis. We have developed a cryogenic reflecting microscope with a numerical aperture of 0.99 and an imaging stability of 0.05 nm in standard deviation at a temperature of 1.8 K. The key optics to realize the cryogenic performances is the reflecting objective developed by our laboratory. With this cryogenic microscope, an individual fluorescent molecule (ATTO647N) at 1.8 K was localized with standard errors of 0.53 nm (x), 0.31 nm (y), and 0.90 nm (z) when 10⁶ fluorescence photons from the molecule were accumulated in 5 min.

Reflecting microscope system with a 0.99 numerical aperture designed for three-dimensional fluorescence imaging of individual molecules at cryogenic temperatures

We have developed a cryogenic fluorescence microscope system, the core of which is a reflecting objective that consists of spherical and aspherical mirrors. The use of an aspherical mirror allows the reflecting objective to have a numerical aperture (NA) of up to 0.99, which is close to the maximum possible NA of 1.03 in superfluid helium. The performance of the system at a temperature of 1.7 K was tested by recording a three-dimensional fluorescence image of individual quantum dots using excitation wavelengths (λ_ex) of 532 nm and 635 nm. At 1.7 K, the microscope worked with achromatic and nearly diffraction-limited performance. The 1/e² radius (Γ) of the point spread function of the reflecting objective in the lateral (xy) direction was 0.212 ± 0.008 μm at λ_ex = 532 nm and was less than 1.2 times the simulated value for a perfectly polished objective. The radius Γ in the axial (z) direction was 0.91 ± 0.04 μm at λ_ex = 532 nm and was less than 1.4 times the simulated value of Γ. The chromatic aberrations between the two wavelengths were one order of magnitude smaller than Γ in each direction.

Spectroscopy of single Pr3+ ion in LaF3 crystal at 1.5 K

Optical read-out and manipulation of the nuclear spin state of single rare-earth ions doped in a crystal enable the large-scale storage and the transport of quantum information. Here, we report the photo-luminescence excitation spectroscopy results of single Pr(3+) ions in a bulk crystal of LaF3 at 1.5 K. In a bulk sample, the signal from a single ion at the focus is often hidden under the background signal originating from numerous out-of-focus ions in the entire sample. To combine with a homemade cryogenic confocal microscope, we developed a reflecting objective that works in superfluid helium with a numerical aperture of 0.99, which increases the signal by increasing the solid angle of collection to 1.16π and reduces the background by decreasing the focal volume. The photo-luminescence excitation spectrum of single Pr(3+) was measured at a wing of the spectral line of the (3)H4 → (3)P0 transition at 627.33 THz (477.89 nm). The spectrum of individual Pr(3+) ions appears on top of the background of 60 cps as isolated peaks with intensities of 20-30 cps and full-width at half-maximum widths of approximately 3 MHz at an excitation intensity of 80 W cm(-2).