Influence of Cementation on the Aesthetical Appearance of Full-Ceramic Restorations

The use of dental ceramics as restorative materials requires corresponding luting materials (cements) that, in turn, influence the visual appearance of the restoration. Due to the high light transmission through the ceramics, the cements can affect the color perception of the dental restoration. This study aims to investigate the optical effects of various cements on the visual appearance of full-ceramic restorations. Three fixing polymer resins (Bifix SE (VOCO GmbH, Cuxhafen, Germany), BreezeTM (Pentron Clinical, West Collins Orange, CA, USA), and PanaviaTM F. 2.0 (Kuraray, Noritake, Osaka, Japan)), with layer thicknesses of 50, 100, 200, and 250 µm, were applied onto a ceramic base model (0.4 mm thick), and irradiated with laser light of wavelengths 532, 632.8, and 1064 nm. Light intensities and scattering effects of light of various wavelengths were angle-dependent, analyzed using a goniophotometer with perpendicular light incidence on the sample specimen (base model plus luting material). In addition, the transmitted power of the light through the sample specimen was determined as a function of the layer thickness. With increasing layer thickness, power losses of respectively 30% for Bifix SE and BreezeTM in the visible spectral range were comparable, whereas PanaviaTM F. 2.0 showed a power loss of ca. 44% here. For the near-infrared range, the power losses for all cements were 25%. This could be confirmed by the interpretation of the line widths. Moreover, the line widths for thin cement layer thicknesses (50 and 100 µm) in the visible spectral range displayed only a redistribution of light by scattering, which does not affect color perception at all. In addition, at 200 and 250 µm, absorption occurred which causes a change in color perception. Within the scope of this study, it could be shown that for thin-layer thicknesses of the cement applied here, there is no adverse optical effect on the aesthetic visual appearance of the restoration.


Introduction
The past years have seen a considerably rising prevalence in metal-free dental restorations, keeping with the trend towards personalized aesthetics. Consequently, the visual appearance in using dental ceramics as full-fledged restorative materials requires establishing corresponding fixing techniques that, on the one hand, compensate for the mechanical stresses and, on the other hand, support optical characteristics. The aesthetics can only then be predicted when the optical interactions of all involved components of the restoration (here, ceramic including the luting cement plus tooth enamel) are considered.

Optical Properties of Restorative Materials
Aligning the restorative materials onto the natural structures is an important aspect regarding aesthetic appearance. Nowadays, the translucency as well as the opacity of ceramic materials can be adapted to the clinical baseline situation. An increase in the crystallization in the matrix causes, for example, an increase in the opacity, thereby allowing a masking of discolored tooth stumps. Variations of the refractive index between the glass and crystalline phases, as well as the crystalline structure, grain size, pigmentation, number, size, and distribution of intrinsic defects, as well as the porosity of the ceramics all influence the light scattering and refraction, which ultimately affect the translucency and opacity and, thus, the light transmission [20]. Moreover, the surface preparation influences the optical properties of the ceramic prosthesis. Heffernan et al. [21] reported about an increase in the translucency of full-ceramic materials after the glazing. Thus, highly translucent silicate ceramics have established themselves in the production of veneers and crowns in the front-tooth area [22]. Consequently, together with the ceramics, the fixing materials need to create a neutral background to ensure the replication of the natural overall appearance.
Using laser light of wavelengths in the visible (VIS) and near-infrared (NIR) spectral ranges, this current work aims to investigate the effects of layer thicknesses of various luting polymers (cements) on the optical properties of full-ceramic restorations. The assumption that the layer thickness of the luting polymers used has no optical influence on the aesthetical appearance of the restorations is defined as a null hypothesis.

Sample Selection and Preparation
Within the scope of this study, three different luting polymers (cements) were chosen: • Bifix SE (VOCO GmbH, Cuxhafen, Germany)-a self-adhesive, polymer-based, dualcure luting cement-consists of bifunctional methacrylates, acidic methacrylates, and inorganic fillers with a filler material fraction of 70% by weight. The selected color shade was "Universal" [23]. • Breeze TM (Pentron Clinical, West Collins Orange, CA, USA) is likewise a self-adhesive, polymer-based, dual-cure luting cement. This cement was used in the color shade "A2" [24]. • Panavia TM F 2.0 (Kuraray, Noritake, Osaka, Japan) is a self-adhesive, polymer-based, dual-cure luting cement in a two-component mixing. The first component contains Methacryloyloxydecyl Dihydrogen Phosphate (MDP)-monomers and a mixture of dimethylacrylates as well as fillers, catalysts, and initiators. The second component likewise consists of dimethylacrylates as well as barium glass and various additives. The total amount of inorganic filling material is approx. 59% by volume. The particle size of the filler ranges from 0.04 µm up to 19 µm. The color shade "Light" was chosen for this study [25].
For determining the optical properties, the cements were applied to a restoration (base) model of a fine-structured feldspathic ceramic. The feldspathic ceramic "Cerec Blocs" (Dentsply Sirona, Charlotte, NC, USA) is characterized, among others, by a high translucency [26], which distinguishes it as a base model for this study. According to the Vitareference, the color 2M2C with the color saturation Medium (M) and the middle brightness (Level 3) was used [26]. With a precision diamond belt saw (EXAKT Advanced Technologies GmbH, Norderstedt, Germany), 45 ceramic discs with a thickness of 0.40 mm ± 0.05 mm could be won as base models from the "Cerec Bloc" (size: 12·14·18 mm). Before the cements were applied, the base models were pretreated on one side with 5% hydrofluoric acid, marketed as VITA CERAMICS ETCH (VITA Zahnfabrik, Bad Säckingen, Germany). Altogether, the combinations of the various cements with the base models subsequently formed the sample specimens for these studies.
For producing the sample specimens with cement thickness layers of 50, 100, 200, and 250 µm, the gap size between two glass plates was measured using a feeler gauge. The cements were mixed according to manufacturer specifications, applied onto the base models, and fixated between both glass plates. By using a polymerization lamp (420-480 nm) of type Acton Mini LED TM Standard (Acton Germany GmbH, Düsseldorf, Germany), the cements were cured at an intensity of 2000 mW/cm 2 and at a total illumination time of 60 s. Here, the illumination took place in two steps, i.e., for 30 s through the glass plate and for 30 s after the glass plate was removed. The final thickness of the sample specimens was examined with an external micrometer of type Mitutoyo IP65 (Mitutoyo Deutschland GmbH, Neuss, Germany). Figure 1 exemplarily shows the sample specimens with a cement layer thickness of 200 µm, presented according to their perceived brightness. For producing the sample specimens with cement thickness layers of 50, 100, 200, and 250 µ m, the gap size between two glass plates was measured using a feeler gauge. The cements were mixed according to manufacturer specifications, applied onto the base models, and fixated between both glass plates. By using a polymerization lamp (420-480 nm) of type Acton Mini LED TM Standard (Acton Germany GmbH, Düsseldorf, Germany), the cements were cured at an intensity of 2000 mW/cm 2 and at a total illumination time of 60 s. Here, the illumination took place in two steps, i.e., for 30 s through the glass plate and for 30 s after the glass plate was removed. The final thickness of the sample specimens was examined with an external micrometer of type Mitutoyo IP65 (Mitutoyo Deutschland GmbH, Neuss, Germany). Figure 1 exemplarily shows the sample specimens with a cement layer thickness of 200 µ m, presented according to their perceived brightness.
Ultimately, 12 samples (three examined materials at four layer-thicknesses) were available for the laser optical studies. A ceramic base model was used as the reference.

Laser Sources
Lasers emitting light of various wavelengths were used for covering a selective color spectrum. The following lasers were used: a frequency-doubled Nd:YVO4 laser of type MGL-III (Changchun New Industries Optoelectronics Tech. Co. LTD., Changchun, China) emitting light of wavelength 532 nm (green) with a maximum power output of 250 mW; a helium-neon laser (He-Ne) emitting light of wavelength 632.8 nm (red) at 5 mW maximum power output (Research Electro-Optics Inc., Boulder, CO, USA); and a Nd:YVO4 laser emiting light of wavelength 1064 nm (near-infrared, NIR) at 1 W maximum power output (Changchun New Industries Optoelectronics Tech. Co. LTD., Changchun, China).

Experimental (Goniophotometer) Setup
Starting from the position of the sample specimen, all optical components such as the laser beam source, beam splitter, imaging and deflection optics, adjusting aperture, and sample and reference detector were aligned in one plane (optical beam path). Beam splitter, adjusting aperture, imaging and deflection optics, as well as the reference detector were positioned fixedly on the optical bench. Depending on the applied source of radiation, the laser beam is coupled in the optical beam path via folding mirrors. The adjusting aperture serves to align the laser beam onto the sample specimen and the Ultimately, 12 samples (three examined materials at four layer-thicknesses) were available for the laser optical studies. A ceramic base model was used as the reference.

Laser Sources
Lasers emitting light of various wavelengths were used for covering a selective color spectrum. The following lasers were used: a frequency-doubled Nd:YVO 4 laser of type MGL-III (Changchun New Industries Optoelectronics Tech. Co. LTD., Changchun, China) emitting light of wavelength 532 nm (green) with a maximum power output of 250 mW; a helium-neon laser (He-Ne) emitting light of wavelength 632.8 nm (red) at 5 mW maximum power output (Research Electro-Optics Inc., Boulder, CO, USA); and a Nd:YVO 4 laser emiting light of wavelength 1064 nm (near-infrared, NIR) at 1 W maximum power output (Changchun New Industries Optoelectronics Tech. Co. LTD., Changchun, China).

Experimental (Goniophotometer) Setup
Starting from the position of the sample specimen, all optical components such as the laser beam source, beam splitter, imaging and deflection optics, adjusting aperture, and sample and reference detector were aligned in one plane (optical beam path). Beam splitter, adjusting aperture, imaging and deflection optics, as well as the reference detector were positioned fixedly on the optical bench. Depending on the applied source of radiation, the laser beam is coupled in the optical beam path via folding mirrors. The adjusting aperture serves to align the laser beam onto the sample specimen and the sample detector. By means of the beam splitter and the imaging optics, the laser radiation is aligned to the reference detector, whereby intensity fluctuations that occur during the measurement can be compensated for. The sample specimen was clamped into the sample holder with a limited amount of spatial mobility. This mobility ensured that the irradiation of the sample specimen on various areas took place respectively under perpendicular incidence of light.
With the help of a stepping motor (C-633 Mercury Step, Physik Instrumente, Karsruhe, Deutschland) and the Software LabVIEW 8.6 (LabVIEW, National Instruments, Austin, TX, USA), the sample detector can be aligned, computer-controlled, at an increment of 0.1 • fully around the sample specimen (360 • ), thus recording the transmitted and reflected light. Photodiodes of type J16-5SP (Teledyne Judson Technologies, Montgomeryville, PA, USA) were used as the reference and sample detectors. Here, this deals with germanium photodiodes which can be used in the wavelength range of ≤600 nm and 1600 nm. At a distance of 13.5 cm between the sample specimen and sample detector and a detector area of 6.6 mm 2 , the light intensity distribution can be spatially detected under an aperture angle of 3 • .

Irradiation Procedure
Power measurements and evaluation: All power measurements were performed with an energy/power meter LabMax Top (Coherent, Santa Clara, CA, USA) combined with a PM10 detector (Coherent, Santa Clara, CA, USA). Moreover, an instrument-internal statistical data or trend analysis allowed the determination of mean and standard deviation values over a timed measurement period.
To ensure the comparability of all measurements, the laser powers of the vanadate lasers were adapted to the output power of the He-Ne laser (5 mW). Within the measuring period of 10 s, the average power was 4.70 mW ± 0.26 mW for all laser systems. Analogously, the measurement was performed on the ceramic base model (thickness 0.4 mm) as well as on every sample specimen with 50, 100, 200, and 250 µm cement thickness including the recording of all mean and standard deviation values. Hereby, the samples were positioned at best closely to the detector area so as to minimize possible scattering losses. Moreover, all sample specimens were irradiated from the ceramic side.

Line Width Measurements and Evaluation
With regard to line shape and line width (Full Width at Half Maximum (FWHM)), conclusions can be drawn regarding the optical properties of the material to be examined. As for the power measurements, all sample specimens were irradiated from the ceramic side. For determining the reflected and transmitted fractions of radiation on the sample specimens as well as on the base model, the sample detector was guided counter-clockwise around the test specimen in 1 • -increments in the angular range of −10 • (Start position) up to 260 • (End position) ( Figure 2).
To exclude manufacturing-related inhomogeneities in the cements, every sample specimen and base model underwent, respectively, four measurements at various spatial positions. By taking into account the number of samples and base model as well as the three laser wavelengths, this resulted in a total of 156 measurements lasting 80 min each. All measurements were conducted in a darkened room so as to rule out external light effects.
All measurement values were recorded as text files and transferred to Microsoft MS Excel 2010 (Microsoft Ireland Operations Ltd., Dublin, Ireland). Mean and standard deviation values were determined for every measurement. OriginPro 8.6 (OriginLab Corporation, Northampton, MA, USA) was used for creating graphs as well as determining the line widths Full Width at Half Maximum (FWHM).

Statistical Evaluation
Descriptive statistics, including calculation of the mean values, standard deviations, and an error estimation, were applied to the power measurements as well as for determining the line width measurements. For data evaluation, Microsoft MS Excel 2010 (Microsoft Ireland Operations Ltd., Dublin, Ireland) was used. The results were evaluated graphically using the spreadsheet calculation program OriginPro 8.6 (OriginLab Corporation, Northampton, MA, USA). Polynomial, exponential, and linear fit functions were used for evaluating and visualizing the data behaviors. To exclude manufacturing-related inhomogeneities in the cements, every samp specimen and base model underwent, respectively, four measurements at various spati positions. By taking into account the number of samples and base model as well as th three laser wavelengths, this resulted in a total of 156 measurements lasting 80 min eac All measurements were conducted in a darkened room so as to rule out external ligh effects.
All measurement values were recorded as text files and transferred to Microsoft M Excel 2010 (Microsoft Ireland Operations Ltd., Dublin, Ireland). Mean and standard d viation values were determined for every measurement. OriginPro 8.6 (OriginLab Co poration, Northampton, MA, USA) was used for creating graphs as well as determinin the line widths Full Width at Half Maximum (FWHM).

Statistical Evaluation
Descriptive statistics, including calculation of the mean values, standard deviation and an error estimation, were applied to the power measurements as well as for dete

Power Measurement/Calibration and Measurement Results
The measurements on the base model enabled an estimation of the influence of the carrier ceramic on the transmission behavior of the entire sample specimen. Figure 3 shows the measured laser output power in air as well as on the base model. Here, the mean transmitted power is 2.65 mW ± 0.50 mW. The ceramic should allow one to expect a uniform attenuation of the laser radiation (parallel shifting to lower laser output powers) over the entire wavelength range. However, the power reductions between the visible (∆P = 2.1 W 532 nm , ∆P = 2.2 W 632 . 8 nm ) and near-infrared radiation (∆P = 1.7 W 1064 nm ) showed clear differences which are also noticeable in the slopes of the linear fit functions. carrier ceramic on the transmission behavior of the entire sample specimen. Figure 3 shows the measured laser output power in air as well as on the base model. Here, the mean transmitted power is 2.65 mW ± 0.50 mW. The ceramic should allow one to expect a uniform attenuation of the laser radiation (parallel shifting to lower laser output powers) over the entire wavelength range. However, the power reductions between the visible (ΔP = 2.1 W532 nm, ΔP = 2.2 W632.8 nm) and near-infrared radiation (ΔP = 1.7 W1064 nm) showed clear differences which are also noticeable in the slopes of the linear fit functions.  Figure 4 shows the influence of the cement layer thickness on the transmitted laser powers for the corresponding laser wavelengths. Since the luting cements were applied onto the base model, the power values for all cement materials lie below the transmission curve of the base model. Moreover, with increasing layer thickness, there is a decrease in the transmitted power for all cements. Over the examined spectral range, an almost parallel power reduction could be observed for all examined materials upon increasing layer thickness. However, for the mean difference values Δ mW, there was a 10-times greater rise in the power from the visible to the near-infrared range for all cements. This illustrates a tendency towards increased transmission behavior of the incident radiation in the near-infrared range (Table 1).  Figure 4 shows the influence of the cement layer thickness on the transmitted laser powers for the corresponding laser wavelengths. Since the luting cements were applied onto the base model, the power values for all cement materials lie below the transmission curve of the base model. Moreover, with increasing layer thickness, there is a decrease in the transmitted power for all cements. Over the examined spectral range, an almost parallel power reduction could be observed for all examined materials upon increasing layer thickness. However, for the mean difference values ∆ mW, there was a 10-times greater rise in the power from the visible to the near-infrared range for all cements. This illustrates a tendency towards increased transmission behavior of the incident radiation in the near-infrared range (Table 1).        Figure 5 shows the line widths for the various wavelengths concerning the base model. The edge effects, described in Figure 2, emerge most prominently at wavelength 532 nm in the area of the line width (FWHM). Even though these edge effects can be likewise seen at wavelengths 632.8 nm and 1064 nm, they do not affect the determination of the line widths. The different manifestation of these edge effects illustrates the angular widening Δ for the various wavelengths. Thus, at wavelength 532 nm, this edge effect occurs in the angular range of 35° and 160° (Δ = 125°). At wavelength 632.8 nm, an angular range of 30° and 170° (Δ = 140°) was determined, whereas an angular range of 20° and 175° (Δ = 155°) was ascertained for wavelength 1064 nm. Realizing this wavelength dependency of Δ532 nm < Δ632.8 nm < Δ1064 nm or conversely for the line widths (FWHM) 116°FWHM @ 532 nm > 71°FWHM @ 632.8 nm > 65°FWHM @ 1064 nm is decisive for the later interpretation of the results.

Line Width Measurements/Calibration and Measurement Results
Since at wavelength 532 nm the line width overlaps with edge effects, the area above the edges were used for measuring the line width (FWHM) ( Figure 5, pink dashed oval). All line widths could be calculated with a polynomial fit of the program OriginPro 8.6.   Figure 5 shows the line widths for the various wavelengths concerning the base model. The edge effects, described in Figure 2, emerge most prominently at wavelength 532 nm in the area of the line width (FWHM). Even though these edge effects can be likewise seen at wavelengths 632.8 nm and 1064 nm, they do not affect the determination of the line widths. The different manifestation of these edge effects illustrates the angular widening Δ for the various wavelengths. Thus, at wavelength 532 nm, this edge effect occurs in the angular range of 35° and 160° (Δ = 125°). At wavelength 632.8 nm, an angular range of 30° and 170° (Δ = 140°) was determined, whereas an angular range of 20° and 175° (Δ = 155°) was ascertained for wavelength 1064 nm. Realizing this wavelength dependency of Δ532 nm < Δ632.8 nm < Δ1064 nm or conversely for the line widths (FWHM) 116°FWHM @ 532 nm > 71°FWHM @ 632.8 nm > 65°FWHM @ 1064 nm is decisive for the later interpretation of the results.

Line Width Measurements/Calibration and Measurement Results
Since at wavelength 532 nm the line width overlaps with edge effects, the area above the edges were used for measuring the line width (FWHM) ( Figure 5, pink dashed oval). All line widths could be calculated with a polynomial fit of the program OriginPro 8.6. Since at wavelength 532 nm the line width overlaps with edge effects, the area above the edges were used for measuring the line width (FWHM) ( Figure 5, pink dashed oval). All line widths could be calculated with a polynomial fit of the program OriginPro 8.6.
According to Figure 1, the luting polymers (cements) were sorted from "light" to "dark" (Bifix SE → Breeze TM → Panavia TM F 2.0). The intensity and the line width diagrams (Full Width at Half Maximum) were likewise analyzed in this order ( Figure 6). For every sample specimen, the line form, averaged over four measurements and depending on the wavelength and the cement layer thickness, was used for determining the respective line width (FWHM). The standard deviation values calculated here were below the 1‰ limit and, thus, were no longer sensibly presentable.
The comparison of the intensity of the measured lines confirms the transmission behavior from the power measurements ( Figure 4) as follows:

•
The light transmission decreases with increasing layer thickness.

•
The light transmission increases with increasing wavelength.

•
The light transmission decreases respectively depending on the material and layer thickness from "light" to "dark".
The first two statements can be clearly verified by the measurement values from Table 2 for all examined cements. The last statement, however, is not fully congruent with the measurement values from Table 2. In the visual spectral range (532 nm and 632.8 nm), Breeze TM , compared to Bifix SE, depicts comparable or lightly increased transmissions. In the near-infrared range (1064 nm), the last statement can again be clearly substantiated. Being the visually "darkest" material, Panavia TM F 2.0 shows the lowest intensities at all cement layer thicknesses and at all wavelengths. According to Figure 1, the luting polymers (cements) were sorted from " stantiated. Being the visually "darkest" material, Panavia TM F 2.0 shows the lowest intensities at all cement layer thicknesses and at all wavelengths.
For the self-adhesive, dual-cure luting polymers Bifix SE and Breeze TM , the line widths (FWHM) show comparable curves at all layer thicknesses, whereas Panavia TM F 2.0, likewise a dual-cure luting polymer but in a two-component mixing, displays considerable deviations in the course of the curves at layer thicknesses of 200 and 250 µ m (Figure 7).  Figure 1 from "light" to "dark" cements, and in the y-axis, the wavelength dependency from short-wave (upper) to long-wave radiation (lower). The layer thicknesses are color-coded in the graphs.  Figure 1 from "light" to "dark" cements, and in the y-axis, the wavelength dependency from short-wave (upper) to long-wave radiation (lower). The layer thicknesses are color-coded in the graphs. Table 2. Measured intensities and line widths (FWHM) as a function of material, wavelength, and layer thickness. The reported intensity values are the maximum values at the measuring angle 100 • of the individual curves from Figure 6. The corresponding line widths were determined according to Figure 5.   The following facts can be expressed for the individual layer thicknesses: • At a layer thickness of 50 µm, it is observed that all luting materials show a clear trend towards a reduction of the line widths from the visual to the near-infrared spectral ranges.

•
The reduction in the line widths at a layer thickness of 100 µm is likewise observed for all luting materials with the exception of Panavia TM F 2.0 which shows a slight increase in the trend curve at wavelength 1064 nm.

Discussion
The goniophotometry represents a proven method for measuring angle-dependent scattered light distributions of a sample specimen. In this context, Jacques et al. [27] mentioned the problems of multiple scattering phenomena at corresponding layer thicknesses. At a layer thickness of the ceramic base model of 0.4 mm, edge effects caused by multiple scattering are clearly recognizable here ( Figure 5). Since scattering represents a wavelength-dependent phenomenon (I ∼ 1 λ 4 ), the edge effects are especially pronounced at 532 nm [28,29]. This was considered during the line width (FWHM) analyses.
According to realistic conditions, all the sample specimens were irradiated from the ceramic side. The losses resulting from the back reflection as well as from the pretreatment with 5% hydrofluoric acid before the cements applied were of a systematic nature and, thus, identical for all sample specimens. Therefore, the influence of surface reflection and scattering based on surface etching could be neglected for all sample specimens.
The laser output powers of the vanadate lasers (532 nm and 1064 nm) were calibrated to the maximum output power of the He-Ne-laser (632.8 nm). The calibration of the vanadate lasers, however, proved itself difficult in its lower power spectrum because of instabilities in the threshold range which resulted in a certain fluctuation margin of the emitted power (Figure 3). The power loss caused by the base models in the visible range was in the order of approximately 52%. In consideration of their wavelengths used, the losses through feldspathic ceramic are comparable with the results of Rasetto et al. [30].

Power and Intensity Measurements
The increase in power and intensity of the transmitted radiation with increasing wavelength (632.8 nm → 1064 nm) was observed for all luting materials and layer thicknesses (Figures 4 and 6). This increase can be explained by the reduced influence of scattering effects towards the near-infrared range (Figure 8).

Power and Intensity Measurements
The increase in power and intensity of the transmitted radiation with increasing wavelength (632.8 nm → 1064 nm) was observed for all luting materials and layer thicknesses (Figures 4 and 6). This increase can be explained by the reduced influence of scattering effects towards the near-infrared range (Figure 8). In general, the sum of all loss mechanisms is designated as extinction ε. In turbid media, absorption and scattering are primary interactions, whereby ε is expressed by the following equation: where µ A is the absorption constant and µ S is the scattering constant. The accompanying intensity losses can be interpreted according to the Lambert-Beer law as: where the term I denotes the transmitted radiation intensity and I 0 the incident radiation intensity, ε the material-intrinsic absorptivity of the attenuating species, and x is the optical penetration depth. Figure 9 exemplarily shows the exponential decrease in power or intensity for Breeze TM at 632.8 nm from the values of Tables 1 and 2.
The various values for ε can be attributed to the differences in the measurement data acquisition. Due to the increased measurement angle for the power measurement at the detector (Power measurements and evaluation), not only the absorption, but also considerable scattering fractions, are detected, which leads to an ε of 0.01 µm −1 according to Equation (1). For the intensity measurement, the extinction results merely in ε = µ A (0.004 µm −1 ), because the data are acquired over a very small spatial angle in the center (measuring angle at 100 • , Figure 2) and, thus, the scattering fractions can be neglected. Consequently, this can explain the various ε-values on hand of the measurement procedure.
where the term I denotes the transmitted radiation intensity and I0 the incident radiation intensity, ε the material-intrinsic absorptivity of the attenuating species, and x is the optical penetration depth. Figure 9 exemplarily shows the exponential decrease in power or intensity for Breeze TM at 632.8 nm from the values of Tables 1 and 2. The various values for ε can be attributed to the differences in the measurement data acquisition. Due to the increased measurement angle for the power measurement at the detector (Power measurements and evaluation), not only the absorption, but also considerable scattering fractions, are detected, which leads to an ε of 0.01 µm −1 according to Equation (1). For the intensity measurement, the extinction results merely in ε = µA (0.004 µm −1 ), because the data are acquired over a very small spatial angle in the center (measuring angle at 100°, Figure 2) and, thus, the scattering fractions can be neglected. Consequently, this can explain the various ε-values on hand of the measurement procedure.
The fundamental material-specific differences can be illustrated from the intensity or line width diagrams ( Figure 6). The luting polymers are composed of their organic polymer matrix, mixed with inorganic fillers and adjuvants such as initiators, catalysts, and inhibitors. The optical properties are enhanced by color pigments and the inorganic fillers. Therefore, the effect on the light interaction is based on the composition of the polymers. For example, the light transmission is affected by the differences in the refractive indices of the polymer matrix and the fillers [32]. Moreover, the monomer type as well as the number, kind, and form of the fillers affect the transmission [33][34][35]. The absorption occurs in the color pigments and/or polymer matrix, whereby the scattering is related to the fillers [36]. The fundamental material-specific differences can be illustrated from the intensity or line width diagrams ( Figure 6). The luting polymers are composed of their organic polymer matrix, mixed with inorganic fillers and adjuvants such as initiators, catalysts, and inhibitors. The optical properties are enhanced by color pigments and the inorganic fillers. Therefore, the effect on the light interaction is based on the composition of the polymers. For example, the light transmission is affected by the differences in the refractive indices of the polymer matrix and the fillers [32]. Moreover, the monomer type as well as the number, kind, and form of the fillers affect the transmission [33][34][35]. The absorption occurs in the color pigments and/or polymer matrix, whereby the scattering is related to the fillers [36].
Bifix SE as well as BreezeTM are self-adhesive luting polymers and show an approximately identical perceived brightness ( Figure 1). Thus, the transmission ( Figure 6) and line width curves (Figure 7) are comparable for all laser wavelengths and layer thicknesses. On the other hand, since PanaviaTM F 2.0 application requires a separate adhesive to the tooth enamel, compared to both other luting polymers, PanaviaTM F 2.0 looks darker and somewhat yellowy (Figure 1). The transmissions seem to be clearly lower ( Figure 6) and the line width curves definitely differ from one another at layer thicknesses 200 µm and 250 µm. Guiraldo et al. [37] reported about the reduction of light transmission at dark colors of conventional polymers, which is associated with increased absorption. The yellowing can be attributed to camphor quinone in the initiator system [38]. Furthermore, the mixing-in of the adhesive may adversely affect the mechanical properties [39]. However, the extent to which the optical properties are affected here is unknown.
The courses of the curves for the various luting materials from Figure 7 can be interpreted by means of Figure 8. Figure 8 principally demonstrates the absorption and scattering behavior in the wavelength range of between 0.5 µm and 10 µm. Hereby, the losses in a logarithmic scale are reflected in the unit dB/km on the y-axis. The interpretations of the courses of the curves from Figure 7 likewise describe the effect of absorption and scattering over the line widths (position and course of the curve as a function of the wavelength) of the transmitted light within the luting materials. Thus, for the applied layer thicknesses used in this work in the µm-range, Figure 8 can be used to make a fundamental assertion about the effects of the loss mechanisms within the luting materials ( Figure 10).
In turbid materials, scattering and absorption normally occur simultaneously but with different weighting, depending on the layer thickness and color. Because of its darker color, Panavia TM F 2.0 shows increased absorption effects already as of a layer thickness of 100 µm (rise in the curves, Figure 7) [37]. By contrast, Bifix SE shows this effect first at a layer thickness of 200 µm. This tendency could not be observed for Breeze TM . als ( Figure 10).
In turbid materials, scattering and absorption normally occur simultaneously but with different weighting, depending on the layer thickness and color. Because of its darker color, Panavia TM F 2.0 shows increased absorption effects already as of a layer thickness of 100 µ m (rise in the curves, Figure 7) [37]. By contrast, Bifix SE shows this effect first at a layer thickness of 200 µ m. This tendency could not be observed for Breeze TM .

Clinical Considerations
The entire visual perception of a full-ceramic restoration is aesthetically influenced, starting from the base (subjacent tooth layer) [15,40] over the luting polymer (cement) and extending to the actual restoration material, the ceramic. The pretreatment of the ceramic and the tooth surface, particle abraded and/or acid etched [19,41], can, based on the created surface structure in combination with the luting polymer, influence the optical as well as the mechanical properties [19] of the full-ceramic restoration. All these aspects are of clinical relevance because teeth as well as the restorative materials are translucent [42].
Especially in the luting polymers, increased scattering effects on the incorporated fillers appear, whereby their size and concentration affect the light scattering [43][44][45]. Moreover, the absorption within the luting polymer increases with increasing layer thickness [43]. Some studies report about changes in the color of full-ceramic restorations depending on the color of the applied luting material [46][47][48][49], whereby the thickness of the applied ceramic exerts a decisive influence. Thus, Vichi et al. [40] observed color differences after cementation at ceramic thicknesses of 1 mm. Therefore, in the application of veneers and crowns in the front-tooth area, a luting polymer may not distort the entire aesthetic impression. Thus, May et al. [50] and Prakki et al. [51] suggest an optimal layer thickness of the luting polymer of between 100 µm and 300 µm, whereas manufacturers specify thicknesses ranging from 10 µm to 30 µm. The present investigations show that at layer thicknesses of 50 µm and 100 µm of all applied luting materials, there is no effect on the aesthetics, i.e., on the color perception, e.g., by absorption in the visible spectral range (Figure 7), which the losses reflect over the averaged line widths in the visible spectral range ( Figure 10). Therefore, the defined null hypothesis had to be rejected for layer thicknesses above 100 µm.
The accuracy in which a restorative procedure can be successfully applied depends on different material (tooth, luting polymer, and ceramic) properties as: translucency [52], color [34,36], thickness [30,53], and shade [49,53], respectively. Adapting the material combinations to the clinical situation shows finally the aesthetical appearance of a fullceramic restoration.

Conclusions
This study illustrates the complex interrelationships in using ceramic materials as full-fledged restoration materials. The tooth base (subjacent tooth layer), luting polymer (cement), and ceramic altogether form a multilayered optical system that affects the whole aesthetic image of the restoration. Ultimately, it could be shown here that the cements applied in thin layers (50 µm and 100 µm) only show a redistribution of light by scattering, which does not cause any impairment in the color perception. Therefore, knowledge about the optical properties of the luting cements and their interaction with light are greatly important for ensuring an aesthetically satisfactory outcome for the restoration. Informed Consent Statement: Experimental study type.

Data Availability Statement:
The data presented in this study are available on request from the corresponding author.