Structural study of polymer hydrogel contact lenses by means of positron annihilation lifetime spectroscopy and UV-vis-NIR methods.

A study has been conducted in order to determine presence of free volume gaps in the structure of structure of polymer hydrogel contact lenses made in phosphoryl choline technology and of the degree of defect of its structure. The study was made by means of positron annihilation lifetime spectroscopy. As a result of the conducted measurements, curves were obtained, which described numbers of counts of the acts of annihilation in the time function. The conducted studies revealed existence of three components τ(1), τ(2) and τ(3). The τ(3) component is attributed to the pick-off annihilation of o-Ps orthopositronium trapping by free volume gaps and provides information about geometrical parameters of the volumes. At the same time, the UV-vis-NIR spectrometry examination was conducted on the same samples in the spectral range 200-1,000 nm.

Introduction

Search for new materials for advanced medical applications, the so called biomaterials, is at present within the range of interest of a large number of scientists: physicists, chemists, biologists, for whom the coincident interdisciplinary approach evolves. Hydrogel materials are modern polymer materials used for making contact lenses, and their chemical and biological properties must be bio-compatible with human organism [1-4].

The objective of the work is making an assessment of physical properties of the polymer material used for making contact lenses by using the positron annihilation lifetime spectroscopy (PALS) method and UV–vis–NIR spectroscopy. In spite of constant improvement of the materials used for making contact lenses, many patients keep suffering from pathological changes in their cornea. There is a need for conducting new studies on properties of polymer materials used for making contact lenses, so as to provide patients with good moistening and appropriate optical parameters, as well as comfort by ensuring their long time use.

Proclear family of contact lenses made by means of the PC technology contain Omafilcon A. The PC technology is based on the assumption that the external layer of the red blood cell membrane is hemocompatible, whereas the internal layer is thrombogenic. The internal, thrombogenic surface has negatively charged phospholipids, while the outer surface is made of closely arranged positively and negatively charges phospholipids, which are, consequently, electrically neutral. 80 % of the external surface of the erythrocyte cell membrane contains phosphoryl-choline, whereas the remaining part is composed of other phospholipids. The smooth PC coating on the surface of contact lenses imitated the bipolar nature of the physiological film and increases bio- and hemo-compatibility. Water molecules also have bipolar structure and this is why many of them are loosely bound on the surface of phosphoryl-choline contained in the contact lenses. Consequently, water molecules bound on the PC surface inhibit binding other molecules and thus reduce the friction factor, which minimize irritation of an eyeball. CooperVision informs that the Proclear family lenses maintain 98 % of water even after 12-h-use. PC covered lenses inhibit formation of bio-film on the surface of the contact lenses. Very little deposit and few bacteria accumulate on the surface (Fig. 1). The biofilm contains diverse microorganisms and extracellular matrix, therefore, it is considered to be as a permanent reservoir of bacteria contributing to development of inflammation of eyeballs.

Fig. 1

Contact lens with a visible reservoir of bacteria

Free positron annihilation is a process involving change of the entire mass of both particles and of their kinetic energy into photon energy of electromagnetic radiation. This is why studying photons formed in the process of annihilation provides information about the condition of the annihilating electron positron pair. Apart from free annihilation, there is also the bounded state annihilation when a positron forms with an electron a hydrogen-like atom called a Ps positronium. The high energy positron annihilation in the matter is preceded by the phenomenon of thermalization, which involves quick loss of positron energy due to scattering and excitation of the medium and thermalization. When losing the last 10–50 eV of its energy a positron covers the distance of the same order and then there may occur a reaction of positronium formation with one of the liberated electrons accompanying, as it were, the positron. Due to different placement of spins, we can distinguish two different types of positronium: para-positronium p-Ps of anti-parallel placement of spins (the 2γ annihilation) and ortho-positronium o-Ps of parallel placement of spins (the 3γ annihilation). Physical properties of positronium change due to its interaction with the surrounding medium. One of the observed phenomena is shortening of three-photon orthopositronium mean annihilation lifetime, which is also called o-Ps annihilation [5, 6]. The basic annihilation process is the “pick-off” annihilation. It involves the ability of the positron, which is part of orthopositronium, to perform two-photon annihilation with one of the atoms that can be found in the surroundings of the positronium [7, 8]. The existence of free volume—an area of zero electron density is necessary for the positronium to survive in a condensed medium without being quenched with a mean lifetime shorter by two orders of magnitude. Local free volumes occur in materials due to irregular molecular packing. In this paper, the Tao–Eldrup model was used to describe the relations between the o-Ps orthopositronium lifetime and the size of a free volume. The model has fully accomplished its task and it has been used for years to calculate the dimensions of free volumes in polymer materials by numerous research centers throughout the world. It assumes that a positronium is trapped within a spherical free volume, is capable of spontaneous annihilation with emission of three γ quanta, or as a result of the pick off process into two γ quanta [9-12].

Experiment

Modern technologies make it possible to produce lenses of better and better parameters that allow using them by children and adolescents by solving problems of dry eyes and tissue reactions to anoxia that occur in hydrogel lenses. They provide possibility for safe use in the case of ageing eyes [13, 14]. The aim of this paper is making an attempt at comparative analysis between individual hydrogel lenses of the Proclear family by means of PALS and UV–vis–NIR spectroscopy. Table 1 shows the family of Proclear contact lenses used in the study.

Table 1

Family Proclear contact lenses used in the study

Sample	Brand	Oxygen permeability: DK/t	Water content (%)	Material Omafilcon A (%)
1	Proclear asphere	28	60	40
2	Proclear sphere	42	62	38
3	Proclear ep	16	60	40
4	Proclear multifocal toric D	42	59	41
5	Proclear multifocal toric N	42	59	41

As described in the preceding paper, measurements of PALS positron lifetimes were taken in room temperature with ORTEC spectrometer, based on the “start–stop” principle. The temporary peak resolution of the measuring system was FWHM = 270 ps. Each sample was formed by 8 layers of contact lenses of 10 mm diameter and 1.2 mm thickness. The examined sample, together with the positron source, which was Na22 sodium isotope of 4 × 105 Bq activity, formed a “sandwich” type system.

Harmful effect of UV radiation to eses and the necessity to use appropriate protection have been discussed for years. Protecting eyes from solar radiation is very important, and this is why additional UV–vis–NIR spectroscopy has been carried out. The UV–vis–NIR spectroscopy is an instrumental technique in which energetic transitions taking place in molecules is used. The transitions are caused by absorption of the electromagnetic radiation in the UV range (200–400 nm), visible range (400–800 nm) or near-infrared range (800–1,000 nm). The technique consists in quantitative measurement of absorption, emission or reflection of light [15].

Tao and Eldrup et al. [10, 11] developed the model in 1972 for free volumes in polymers. They pondered over a simple model in which the Ps atom is located in a finite, spherical potential trough. In order to simplify calculation, replacement of the finite potential trough by an infinite potential trough, extended by the ΔR value. It is necessary for reconstruction of the values of probability of finding o-Ps outside the potential trough of finite depth and radius R. Successive theoretical deliberations showed that τ3 o-Ps lifetime expressed as a function of radius R free volume is expressed by the formula:where ΔR = 0.166 nm is the fitted empirical electron layer thickness. By fitting the above equation with the measured τ3 values, R and free volume size Vf as:can be evaluated. The relative intensity of the longest component I3, is generally correlated to the density of the holes, which can be considered as a kind of trapping centres for Ps. A semi-empirical relation may be used to determine the fraction of free volume (fv) in polymers as:where: Vf—is the free volume calculated from τ3, using Eq. (1) with a spherical approximation, I3—(in %) is the intensity of long-lived component, C—is empirically determined to be 0.0018 from the specific volume data [5].

In the further part of the study, a two-state model of positron annihilation was proposed for the analysis of PALS spectra. In this model, a positron annihilates from the free state and from one state localized in a defect, without the detrapping process. After calculating, with the use of the LT program, the major annihilation parameters—mean positron lifetimes τ1, τ2 and their intensities, we can also calculate [16]:

Mean positron lifetime τav illustrating defectiveness of the dominant medium in the examined lenses;

Mean positron lifetime in an unidentified structure τb;

Capture speed of positrons by traps (defects) κd; —the magnitude connected with means size of defects in which annihilation occurs, —illustrating the type of volume defects.

A model experimental curve of the spectrum of positron lifetime in a contact lens sample is shown in Fig. 2.

Fig. 2

The spectrum of positron lifetime in a contact lens sample

The UV–vis–NIR spectrometric testing was carried out with an OceanOptics high-resolution HR 4000CG-UV–NIR spectrometer in the spectrum range 200–1,000 nm. A deuterium–tungsten-halogen lamp, covering the spectrum range of the spectrometer used in the study was used as a source of light. The power of the source of light was 3.8 W (deuterium lamp) and 1.2 W (tungsten-halogen lamp). The transmission spectra for the examined contact lenses are shown in Fig. 3. The graph shows that the examined lenses stop ultraviolet radiation.

Fig. 3

UV–vis–NIR transmission spectra for the examined contact lenses

Results and discussion

Positron lifetime spectra were analysed with the LT computer program [17]. Results of calculation of values of mean lifetimes of positrons in the examined samples revealed existence of three components, τ1, τ2 and τ3, in the positron lifetime spectra. In our earlier publications on the topic we concentrated on analyzing only τ3, the third component of positron lifetimes [18]. This time we additionally analyse the components τ1 and τ2, which concern the two-state model of positron annihilation. Mean positron lifetime values τ1, τ2, τ3 and their intensities are shown in Table 2.

Table 2

Mean positron lifetime values τ1, τ2, τ3 and their intensities

Sample	τ1 (ns)	I1 (%)	τ2 (ns)	I2 (%)	τ3 (ns)	I3 (%)
1 asphere	0.207 ± 0.006	76.03 ± 1.56	0.580 ± 0.034	18.23 ± 1.60	1.800 ± 0.180	5.75 ± 0.35
2 sphere	0.180 ± 0.006	63.06 ± 0.97	0.476 ± 0.010	31.12 ± 0.97	1.803 ± 0.024	5.80 ± 0.19
3 ep	0.211 ± 0.007	68.05 ± 1.45	0.533 ± 0.022	24.90 ± 1.53	1.822 ± 0.028	7.07 ± 0.30
4 multifocal toric D	0.230 ± 0.005	71.34 ± 1.34	0.517 ± 0.054	24.01 ± 1.43	1.853 ± 0.075	4.66 ± 0.17
5 multifocal toric N	0.235 ± 0.005	76.17 ± 1.43	0.564 ± 0.089	20.07 ± 1.47	1.893 ± 0.066	3.79 ± 0.26

The obtained errors are the result of mathematical analysis. Positron lifetime values τ3 o-Ps (the “pick-off” process) and their intensity I3, as well as the dimensions of free volumes R are displayed in Table 3.

Table 3

Mean positron lifetime values τ3, their intensity I3 and sizes of free volumes

Sample	τ3 (ns)	I3 (%)	R (nm)	Vf (10−30 m3)	fv (a.u.)
1 asphere	1.800	5.75	0.265	77.92	448.04
2 sphere	1.803	5.80	0.266	78.80	457.04
3 ep	1.822	7.07	0.268	80.59	569.77
4 multifocal toric D	1.853	4.66	0.271	83.33	388.32
5 multifocal toric N	1.893	3.79	0.275	87.08	330.03

The free volumes dimensions Vf and the fraction of free volumes Vf × I3 = fv/C for all the examined samples are displayed in Figs. 4 and 5 respectively.

Fig. 4

The average size of free volume Vf for samples of contact lenses: 1 proclear asphere, 2 proclear sphere, 3 proclear ep, 4 proclear multifocal toric D, 5 proclear multifocal toric N

Fig. 5

The fractional of free volume fv/C for samples of contact lenses: 1 proclear asphere, 2 proclear sphere, 3 proclear ep; 4 proclear multifocal toric D, 5 proclear multifocal toric N

The fraction of free volume fv is proportional to Vf × I3, because C in the Eq. (4) is constant. There are values of τ1 and τ2 positron lifetimes and their intensities, as well as the determined parameters of positron capture for the examined samples of contact lenses presented in Table 4.

Table 4

Calculated values of positron lifetime and positron capture of the examined samples of contact lenses

Sample	Fitting parameters						Parameters of positron capture
	τ1 (ns)	I1 (%)	τ2 (ns)	I2 (%)	τ3 (ns)	I3 (%)	τav (ns)	τb (ns)	κd (ns−1)	τ2−τb (ns)	τ2/τb (ns)
1	0.207	76.03	0.580	18.23	1.800	5.75	0.279	0.236	0.603	0.344	2.458
2	0.180	63.06	0.476	31.12	1.803	5.80	0.278	0.226	1.146	0.250	2.106
3	0.211	68.05	0.533	24.90	1.822	7.07	0.297	0.252	0.766	0.281	2.115
4	0.230	71.34	0.517	24.01	1.853	4.66	0.302	0.267	0.610	0.250	1.936
5	0.235	76.17	0.564	20.07	1.893	3.79	0.304	0.268	0.515	0.296	2.104

Changes of τ3 life time values and their intensities I3 are presented as changes of free volumes Vf and numbers of free volumes fv (Figs. 4, 5). It results from Fig. 4 that each sample is characterized by a different Vf value. As for the fv parameter, responsible for changes of free volume numbers occurring in the examined contact lenses, there are certain similarities. There are values close to fv in the Asphere and Sphere lenses, another pair are the Multifocal Toric D and Multifocal Toric N lenses. The EP lens, on the other hand, is distinguished by an indirect value for both Vf and fv parameters. It is possible to look for connections with the optical properties of the contact lens. According to CooperVision, the lens is “something in between” ordinary lenses for correcting far-sightedness and multifocal lenses, and it is generally used to correct presbyopia in young people.

When analyzing results of the study (Table 4), it is noticeable that there is a relation between the percentage of Omafilcon content and τ1 responsible for free annihilation of positrons and the annihilation with electrons of point defects of vacancy type. Two contact lenses, Multifocal Toric D and Multifocal Toric N stand out as having the highest τ1 values and the highest Omafilcon content (41 %). The same relation can also be found for the mean positron lifetime τav reflecting defectiveness of the medium for the same contact lenses. Apart from that the lenses Multifocal Toric D and Multifocal Toric N also stand out because of highest values of τb. Analysing subsequent parameters of positron capture, one can observe that the highest speed of positron capture by the κd traps (defects) is demonstrated by the Sphere lens, whereas the lowest speed is demonstrated by the Multifocal Toric N lens. The parameter τ2−τ1, i.e. mean defect sizes is the highest for the Asphere lens and the lowest for the Sphere and Multifocal Toric D lenses. Differences for the τ2/τ1 parameter can be observed, which is evidence of geometric variability for individual contact lenses.

Conclusions

This paper deals with a study on determining occurrence of free volume vacancies in the structure of polymer hydrogel contact lenses made by means of PC technology by CooperVision and on the degree of defectiveness of the structure by means of the PALS method.

As a result of the conducted studies and calculations of positron lifetime spectra values of three τ components (τ1 short-lived, τ2 average-lived, and long-lived τ3 o-PS) and their intensities I have been obtained. The results of these measurements show that formation of free volume vacancies takes place in all contact lenses of the Proclear family. In spite of the fact that all the examined contact lenses are made of the same polymer material (Omafilcon), the designated parameters vary. The calculated values of dimensions of Vf free volumes and the fraction of fv free volumes show that the highest values of Vf occur in Multifocal Toric D and Multifocal Toric N lenses, and at the same time the lowest fv values are observed for the same contact lenses.

As for the positron capture parameters (the degree of defectiveness of the structure), Multifocal Toric D and Multifocal Toric N contact lenses show the highest defectiveness of the medium, but at the same time a low speed of defecting positrons. However, the same type of positron trapping forms in all cases, and the differences in results confirm structural changes in contact lenses resulting from their technological modification.

There arises one basic conclusion from the UV–vis–NIR study, which indicates that all the examined contact lenses from the CooperVision Proclear family stop harmful ultraviolet radiation.