Abstract
Such samples are usually unique and irreplaceable. Hence, cells leaving long-term storage cannot be globally tested for physiological and genetic soundness before their medical application. Therefore, it is obligatory to ensure a damage-free long-term storage. Once aqueous samples have reached a temperature below −137°C, they are considered to be stably cryopreserved, as this is the glass transition temperature (Tg) of amorphous water and no ice crystal formation should occur below Tg. Furthermore, chemical and biological activity and diffusion virtually stop below this temperature. These aspects are particularly important with respect to vitrified samples which have solidified in a metastable, amorphous (glassy) state by sudden cooling. Ice formation in vitrified samples due to transient infringing of the Tg usually leads to loss of the complete sample.1,2 Furthermore, mechanical and thermal incidents may occur without notice in biobanking practice (e.g., when moving single specimens or entire sample collections). An interrupted cold chain may have ruinous effects on a sample, but currently is not traceable before rewarming. Against this background, it is remarkable that still no quality monitoring of long-term stored samples is conducted at present, neither
We set up a fiber-based Raman probe for a proof-of-concept experiment. A Cryostage (CS) (Linkam MDS 600, Linkam Scientific, UK) served as a mimic for the sample (S) during cryogenic storage. The sensing setup consists of confocal probe interface (CPI), connected via fiberoptics to a dichroic fiber junction (DFJ), as well as a fiber-borne CCD-spectrograph (Fig. 1a). The confocal probe interface is a combination of a fiber coupler and a focusing optic. The dichroic fiber junction couples a free beam laser (532 nm, Coherent Compass, USA) via beam expander (BE), dichroic beam splitter (DBS), and a fiber coupler into the probe fiber (PF). The Raman light coming back from the probe fiber is collected by the same fiber coupler, separated from excitation light by the dichroic and a long-pass filter (LP, Razoredge, Semrock) and a coupled-into-the-detection fiber (DF). The collected Raman light is spectrally detected by a fiber-borne spectrograph assembly (iDus CCD-detector with Shamrock 303 polychromator (Andor Technology plc., UK).

For a microscopic investigation of the crystallization, the Raman technology was adapted to a sample-scanning confocal microscope with the Linkam stage as cryogenic microscopy chamber. Mounting the cryo-chamber on a xy-sample-scanner (Physik Instrumente, Germany) of 300 μm traveling distance enables Raman spectral imaging (Fig. 1b). Image reconstruction was performed by an in-house-developed Labview Software.
Scanning Raman microscopy was performed in order to identify the origin of spectral bands using the setup shown in Figure 1b. Each pixel of such a microscopy image contains an entire Raman spectrum. By subsequent data analysis, images of arbitrary spectral channels can be generated displaying isolated molecular vibrations (i.e., chemical compounds). Hence, Raman microscopy enables one to measure and map the concentration as well as the chemical state of the main constituents of a sample. To resemble typical slow freezing conditions, we cooled a single suspended human mesenchymal stem cell (hMSC) down to −120°C at a rate of −1 K/min in a PBS solution containing 10% DMSO. The respective Raman images of three isolated vibrations are shown in Figure 2a and the corresponding spectral data are plotted in Figure 2b. In Figure 2a, concentration maps of cellular matter (measured as hydrocarbon backbone vibration C3), ice (measured as lattice OH stretching vibration), and DMSO (measured as C-S-stretching vibration) of a hMSC slowly frozen to −120°C are shown. Figure 2b displays the respective spectra of pixels from the cellular body, extracellular ice phase, and dendritic fluid channels (residual extracellular liquid phase), and further denotes the vibration bands used for the chemical mapping in Figure 2a. The contrast mechanisms of low temperature confocal Raman microscopy are described elsewhere in detail.7,8 The O-H stretching vibration region beyond 3000 cm-1 differs significantly between the crystalline and amorphous states of water (Fig. 2b). This distinct difference in spectral shape was used to monitor recrystallization in vitrified samples as described in the next paragraph.

In order to prove the concept of monitoring recrystallization of vitrified samples during cold storage, we mimicked a measured typical temperature profile of a sample vial while a neighboring vial was withdrawn from the cryocontainer. The process was monitored with a remote sensor setup (Fig. 1a) using 2 μL glassy vitrification medium (without cells) in the Linkam stage (vitrification medium: PBS (300 m

A series of Raman spectra from a sample mimic heated from −141°C to −100°C, indicating the formation of ice at −127°C by the occurrence of the characteristic ice band at 3120 cm−1. Exemplary Raman spectra of glassy water and ice are shown on the
Ice formation and the application of cryoprotective substances in cryopreserved samples can be unambiguously detected at cryogenic temperatures by fiber-based Raman spectroscopy. Furthermore, this technique allows a differentiation between CPA as well as freezing protocols used, such as vitrification or slow freezing. As this technique is moreover capable of detecting any other chemical change in principle, it turns out to be a powerful method for contact-less monitoring of the status of cryopreserved samples during storage. The technical implementation of the concept may lead to automated monitoring of samples under cryogenic storage in the future. However, the storage technology has to allow transport of samples to the optical interface inside the cryo-tank. The optical interface and sample container have to be designed in a way that allows a representative measure (i.e., a multisport or widefield measure). Such efforts will be made only for very valuable samples. A short-term implementation into biobanking practice is the spectroscopic pre- and post-storage sample characterization in cryogenic temperature workbenches to check for chemical changes during the conservation and for ice formation in vitrified samples. A quality assessment for sample transportation can also be performed this way. The confocal optics of the present fiber probe already allows measurements through turbid container walls, as was tested on Teflon straws. A multispot confocal probe for workbench application is in development at the moment. Raman spectroscopy could be used to develop catalogue references for quality management of cryopreserved samples. Comparison to catalogued spectra may enable retrospective sample analysis.
Footnotes
Acknowledgments
The authors are grateful to Uwe Schön for the allocation of the measuring data of the temperature gradients of the sample recovery from a state-of-the-art cryo-tank, and to Axel Beier for compounding the vitrification media. We also thank Martin Schwarz for his work on the Labview-based image-acquisition software, and Dr. Stephen Shirley for helpful discussions and critical review as regards content and language. Finally, we would like to thank Hanna Lorig for cell culture and providing the hMSC. The hMSC were isolated from Wharton's Jelly of umbilical cord with informed consent of the mother.
Author Disclosure Statement
This work was supported by the Fraunhofer Society. No competing financial interests exist.
