1. INTRODUCTION
Three-dimensional (3D) printing technology has begun to advance rapidly across various
industrial sectors. Ceramic 3D printing has gained significant attention because of
its ability to overcome the inherent limitations of mold-based manufacturing, including
high cost, extended production time, and constraints in shape realization [1].
Among various techniques, digital light processing (DLP) has emerged as a promising
method for fabricating high-precision ceramic components, including biomedical implants
[2,3]. It also minimizes the need for postprocessing, such as, precision machining [4], thereby enabling the direct fabrication of complex and high-precision components.
This approach utilizes a slurry composed of ceramic powders dispersed in a photocurable
resin, which allows the construction of fine structures with high resolution and holds
great industrial potential. Commercialization of oxide-based ceramics such as Al2O3 and ZrO2 has been achieved and ongoing improvements are being made in process reliability
and technological maturity. However, nonoxide ceramics such as silicon nitride (Si3N4) present several challenges DLP-based ceramic 3D printing applications. In particular,
the ability to fabricate high-strength Si3N4 spinal implants remains difficult due to the formulation constraints of photocurable
slurries [5]. The Si3N4 slurry must maintain a high solid loading while also remaining photocurable and stable
during printing. Therefore, precisely optimizing slurry formulation is essential.
Silicon nitride is a representative non-oxide ceramic that has gained considerable
research attention not only for applications in the aerospace, automotive, and electronic
industries but also as a promising material for orthopedic implants, thanks to its
high flexural strength, excellent fracture toughness, superior wear and corrosion
resistance, and biocompatibility [6,7]. Si3N4 exhibits superior antibacterial properties, X-ray transparency, and bioactivity compared
to conventional spinal implant materials such as titanium (Ti) and polyetheretherketone
(PEEK), These features, make it a potential a next-generation material for spinal
interbody fusion devices known as spinal cages [6,7].
Commercial Si3N4 spinal cage products are currently manufactured, particularly in the United States,
using traditional press molding and high-temperature sintering methods and are carefully
evaluated for osteoconductivity and antibacterial activity. The conventional manufacturing
processes have difficulty producing complex geometries, and often requires costly
machining and post-processing to achieve the final shape, resulting in increased process
complexity and manufacturing costs.
Spinal cages are widely used as orthopedic implants to treat spinal diseases such
as spinal stenosis, herniated discs, and facet joint hypertrophy, and their use has
become more prevalent in aging populations. These implants are inserted between adjacent
vertebral bodies after removing a damaged disc to restore intervertebral height and
spinal curvature while providing biomechanical stability. Recently, with the increasing
demand for personalized spinal cages and complex designs, DLP-based 3D printing has
emerged as a viable technology for high-precision fabrication. Si3N4 has attracted renewed interest as an advanced biomaterial that can combine high mechanical
strength, bioactivity, and antibacterial properties [8].
Si3N4 exhibits excellent cell compatibility, which promotes the adhesion and differentiation
of osteoblasts on its surface [9], and it demonstrates no cytotoxicity. Because of its strong antibacterial properties,
potential applications in the fields of orthopedics and dental implants are continuously
expanding. However, fabricating complex geometries and ensuring repeatability and
dimensional precision is challenging for traditional press molding and machiningbased
processes. In contrast, DLP-based ceramic 3D printing is attracting attention as a
next-generation technology for fabricating Si3N4 implants because of its ability to accurately reproduce intricate and fine structures
while reducing the number of processing steps.
Photopolymerizable ceramic slurries play a central role in DLP-type ceramic 3D printing.
This type of slurry, consisting of ceramic powders uniformly dispersed in a photocurable
resin matrix, directly affects the printing resolution and final mechanical properties
of sintered parts. Importantly, it is often difficults to achieving high solid loading
while maintaining suitable viscosity, dispersion stability, and photopolymerization
reactivity because these requirements are often mutually conflicting. For example,
insufficient photoinitiator content can result in incomplete curing, which can lead
to weak interlayer adhesion and poor printing stability. Conversely, excess photoinitiator
can increase polymerization shrinkage, which can cause warpage or delamination during
the printing process. Further, excessively high slurry viscosity can hinder recoating
and smooth spreading, while excessively low viscosity can lead to particle sedimentation
and poor homogeneity.
To address these challenges associated with photopolymerizable ceramic slurries, this
study systematically investigated the effects of binder components, namely, the blending
ratio of monomers A and B, content of the photoinitiator, oligomer addition levels,
and dispersant concentration, on the rheological behavior and printability of the
slurry. Monomer A provides favorable viscosity control and low polymerization shrinkage;
however, it exhibits slower curing kinetics. In contrast, monomer B cures rapidly
and contributes to higher mechanical strength; however, it can cause internal stresses
and interlayer delamination. Therefore, a mixed monomer system was explored to balance
the advantages and mitigate the drawbacks of each component. The photoinitiator, which
governs both the curing depth and viscosity, also requires optimization to ensure
effective photopolymerization. Oligomers reduce polymerization shrinkage and enhance
mechanical strength; however, their high molecular weights can significantly increase
slurry viscosity, which necessitates careful formulation to achieve a balance between
mechanical performance and flowability. Dispersants, although effective at preventing
particle agglomeration and enhancing dispersion stability, can negatively affect the
photopolymerization reaction if used excessively.
Given this context, this study aims to evaluate the rheological and photopolymerization
characteristics of Si3N4 photopolymerizable slurries with varying compositions and identify optimal conditions
for increasing solid loading while maintaining dimensional stability and processability.
Subsequently, the optimized slurry system was employed to fabricate prototype spinal
cage components via DLP 3D printing. Postprocessing included debinding and gas pressure
sintering under a nitrogen atmosphere, followed by mechanical performance evaluations
to verify the viability of DLP-based Si3N4 manufacturing for high-performance orthopedic implants. Further, a DLP-compatible
Si3N4 slurry system was developed in this study that can enable both high solid content
and stable layer-by-layer fabrication by optimizing the formulation of the binder
constituents. The effects of the monomer A/B blending ratio on rheological stability
and curing behavior were examined, and the effects of photoinitiator content on the
viscosity and cure depth were assessed. The trade-off between viscosity control and
mechanical enhancement was addressed by tuning the type and dosage of the oligomers,
and the dispersant level relative to the ceramic content was calibrated carefully.
Subsequently, the feasibility of manufacturing spinal cage prototypes was validated
by printing, debinding, and nitrogen sintering, demonstrating the applicability of
the proposed formulation strategy for advanced ceramic implant production via DLP.
2. EXPERIMENTAL
2.1 Starting Materials
A photopolymerizable Si3N4 slurry suitable for DLP-based ceramic 3D printing was prepared and optimized in this
study. The primary ceramic powders used in the slurry formulation included Si3N4 (SN-E10, UBE Corp., Japan), Al2O3 (AKP-53, Sumitomo Chemical, Japan), and Y2O3 (Yttrium oxide, Sigma-Aldrich, USA). The average particle sizes of these powders
were confirmed to be 1.67, 0.192, and 1.099 μm for Si3N4, Al2O3, and Y2O3, respectively.
The ceramic composition was initially set to a weight ratio of Si3N4:Y2O3:Al2O3 = 90:5:5 based on previous studies and literature reports [10]. This composition was selected to facilitate the α-phase to β-phase transformation
of Si3N4 and promote densification during sintering [11]. Sintering additive ratios were slightly adjusted following mechanical property
evaluations; however, the final optimized composition remained consistent at Si3N4 90 wt%, Y2O3 5 wt%, and Al2O3 5 wt%.
A photocurable resin system was formulated using two commercially available acrylate-based
monomers with distinct viscosities: monomer A, Isobornyl Methacrylate (240 cP), which
is a monofunctional monomer primarily used for viscosity control and to achieve a
more moderate curing speed, and monomer B, Trimethylolpropane Trimethacrylate (TMPTMA)
(76 cP), a highly reactive trifunctional monomer chosen for its ability to form a
high crosslinking density network, thus ensuring rapid curing and enhanced mechanical
properties of the cured layers.. To enhance the interlayer adhesion and uniformity
of the cured resin while precisely regulating the slurry viscosity, two types of urethane
acrylate-based oligomers were blended into the formulation. High-viscosity oligomer
A (4,560 cP) is a hexafunctional urethane acrylate oligomer, incorporated to achieve
low shrinkage upon curing and a high crosslinking density, thereby contributing to
improved durability and the dimensional precision of the final parts. However, its
high functionality can lead to increased brittleness. Conversely, low-viscosity oligomer
B (384 cP) is a difunctional urethane acrylate oligomer, primarily added to enhance
interlayer adhesion and mitigate the brittleness associated with oligomer A, while
also assisting in viscosity control. A photoinitiator (Irgacure 819, BASF, Germany)
was used, as well as Dispersant (BYK-110, BYK, Germany) to ensure the stable dispersion
of the ceramic powders within the slurry.
2.2. Slurry Formulation and Preparation
Nine photocurable resin compositions were designed and categorized into three groups
to optimize slurry formulation: M-A, M-B, and M-AB. These formulations were prepared
by varying the photoinitiator content (2, 3, and 4 wt%) and weight ratio of monomers
A and B. The curing characteristics and layer-by-layer printing stability were evaluated
for each formulation. A constant 50 wt% loading of Si3N4 powder was used in each composition to measure the curing depth, and the most suitable
monomer composition for layer-by-layer DLP processing was selected based on these
results.
The slurry was prepared using a two-step mixing process: The monomer–oligomer mixture,
ceramic powder, and dispersant were premixed using a planetary mixer (Thinky Mixer
ARE-310, Thinky Corp., Japan) at 500 rpm for 10 min. Subsequently, the resulting premix
was transferred to an attrition mill (Netzsch, Germany), where it was further dispersed
at 500 rpm for 30 min using zirconia beads as the milling medium. This dispersion
step was intended to eliminate agglomerates of the ceramic particles and ensure a
homogeneous slurry. Following mixing, the slurry was subjected to vacuum degassing
for 10 min to remove entrapped air bubbles.
The rheological properties of the slurry were measured at 25 °C using a rotational
viscometer (Brookfield DV2-Pro) immediately after preparation and again after 24 h
of ambient storage. The measurements were conducted at sufficiently low shear rates
considering the inherently high viscosity of the slurries. The variation in viscosity
over time was used to assess the stability of each formulation. Further, the effects
of oligomer content on slurry viscosity and cured body (green body) strength were
systematically investigated. In this series of experiments, monomer A was used exclusively
(M-A series), and the content of high-viscosity oligomer A was increased incrementally
from 0 to 10 wt%. The slurry viscosity, printability, and three-point bending strength
of the cured bodies were measured for each composition.
These results confirmed that the addition of 8 wt% oligomer A produced the most favorable
balance between mechanical strength and printability. Subsequently, partial replacement
with the low-viscosity oligomer B was explored to mitigate the increase in viscosity
associated with oligomer A. The total oligomer content was fixed at 8 wt%, and the
ratio of oligomers A to B was varied from 8:0 to 3:5. The viscosity and mechanical
strength of each formulation were compared, and the optimal oligomer combination was
identified.
2.3. Printing and Evaluation Process
A custom-built DLP 3D printer was utilized to evaluate the curing behavior and layer-by-layer
printing characteristics of the photocurable slurry. The system employed a 405 nm
wavelength ultraviolet light emitting diode (UV-LED) projector as the light source,
with an XY resolution of 40 × 40 μm and a build platform size of 50 × 50 mm. The printing
process was conducted in a bottom-up configuration, and the layer thickness was set
to 50 μm.
Prior to printing, the curing depth of each slurry composition was measured, and this
confirmed controllable depths in the range of 25–60 μm. It was determined that an
energy dose of ~1000 mJ/cm2 was required per layer under the 50 μm condition. Accordingly, each layer was exposed
to the same energy dose during printing. After each UV exposure, the build platform
was raised by 50 μm, followed by the application of a new slurry layer and subsequent
pattern exposure in a repeated cycle. The photocurable resin system undergoes a free
radical chain-growth polymerization mechanism upon UV irradiation during the printing
process. This fundamental chemical reaction proceeds in three main steps:
Initiation Step: A radical (R·) generated from the photoinitiator by UV exposure reacts
with the double bond of an acrylate or methacrylate, initiating the polymerization.
Propagation Step: The newly formed radical continuously reacts with the double bonds
of other monomers, leading to extension of the polymer chain.
Termination Step: The polymerization reaction concludes when two radicals combine,
forming a crosslinked polymer network.
During the printing process, slurry spreadability, interlayer adhesion, and deformation
caused by curing shrinkage were monitored in real time to evaluate the printing stability
of each formulation. After printing was completed, the dimensional accuracy and morphological
stability of the cured specimens were assessed by comparing the printed shapes against
the CAD model, with particular attention to warping and cracking.
The printed green parts were subjected to a post-curing process at 50 °C for 1 h,
followed by a multistep debinding and sintering treatment. The debinding profile was
determined using thermogravimetric analysis (TGA), which identified the decomposition
range of the organic components. Further, the temperature was increased from 25–400
°C at a ramp rate of 1 °C/h to ensure the complete removal of organics.
Sintering was performed in a nitrogen (N₂) atmosphere at temperatures ranging from
1,700–1,900 °C, with a holding time of 2 h. Atmospheric pressure sintering and gas
pressure sintering (GPS) were applied for comparison. Although atmospheric sintering
was conducted under ambient N2 pressure, the GPS was conducted under 1 MPa N2 at both
1,800 and 1,900 °C. The mechanical properties of the sintered bodies were evaluated
using three-point bending strength, Vickers hardness, and fracture toughness. The
flexural strength test was conducted at room temperature in accordance with KS L ISO
14704, and the Vickers hardness was determined from the five measurements of polished
surfaces in accordance with KS L ISO 14705. Fracture toughness was estimated based
on the fracture characteristics of the specimens.
3. RESULTS & DISCUSSION
3.1. Effect of Monomer Composition and Photoinitiator Content
In the DLP 3D printing process, the viscosity of the ceramic slurry is a key parameter
that determines both stacking stability and the dimensional precision of printed structures.
A slurry with an excessively low viscosity can result in sedimentation of the ceramic
particles, which leads to layer-wise inhomogeneity and printing defects [12]. In contrast, an excessively high viscosity can reduce slurry flowability, which
results in poor coating and process delays [13]. this study investigated, the effects of monomer composition and photoinitiator
content on slurry viscosity and time-dependent stability.
The effect of photoinitiator content was evaluated using monomer-A-based formulations
(M-A series, 60 wt% ceramic). Fig 1(a) shows that increasing the photoinitiator content from 2−4 wt% led to a gradual decrease
in the initial slurry viscosity. This trend is attributed to the partial action of
the photoinitiator as a solvent-like component, which reduces the overall viscosity
of the system [14]. For example, the viscosity decreased from ~12,500 cP at 2 wt% to ~10,800 cP at
4 wt%. However, the rate of viscosity reduction diminished above 4 wt%, and the excessive
addition of photoinitiator resulted in solid dilution and undesirable curing shrinkage.
Therefore, the 3 wt% was selected as an optimal concentration to balance curing efficiency
and viscosity control.
Further, the time-dependent stabilities of different monomer formulations were compared.
For the M-A-3 and M-B-3 formulations that comprised monomers A and B, respectively,
M-A-3 showed the lowest initial viscosity but exhibited more than a 20% viscosity
increase after 24 h, which implies reduced temporal stability. In contrast, M-B-3
had a slightly higher initial viscosity; however, it maintained good stability with
less than a 5% change over the same period. The mixed monomer formulation M-AB-3 (A:B
= 1:1 by weight) exhibited an intermediate initial viscosity of ~11,400 cP and the
highest temporal stability, with less than a 3% increase after 24 h, as shown in Fig 1(b). These results are consistent with previous studies, which report that monomer A
tends to undergo phase separation or aggregation over time, thereby increasing viscosity
while the highly reactive monomer B promotes early partial network formation, stabilizing
the slurry [15]. The observed differences in viscosity and stability with the monomer formulations
(M-A-3, M-B-3, M-AB-3) are not solely due to the inherent viscosity differences of
monomer A (240 cP) and monomer B (76 cP), which contribute to a dilution effect. More
critically, the distinct chemical functionalities of these monomers govern the photopolymerization
kinetics and the resultant polymer network structure. Monomer A, being a monofunctional
Isobornyl Methacrylate, contributes to viscosity control and a moderate curing speed,
but its limited crosslinking capability results in a less rigid network, potentially
leading to the observed higher viscosity increase over 24 h and post-printing warpage.
In contrast, monomer B, Trimethylolpropane Trimethacrylate (TMPTMA), is a highly reactive
trifunctional monomer that facilitates the rapid formation of a highly crosslinked
polymeric network. This dense network contributes to faster curing and improved initial
stability, but can induce higher polymerization shrinkage, causing delamination. Therefore,
the optimal mixed monomer formulation (M-AB-3) leverages both the viscosity-reducing
effect of monomer B and the balanced crosslinking capability offered by the combination
of monofunctional monomer A and trifunctional monomer B. This synergistic blend effectively
harmonizes curing shrinkage, viscosity, and printing quality, leading to superior
dimensional stability and print reliability.
In addition, stacking experiments were conducted using a DLP 3D printer for all nine
resin formulations listed in Table 1. For the M-A series composed solely of monomer A, no significant deformation occurred
during the stacking process. However, after printing, warping was observed at the
edges of specimens as depicted in Fig 2(a). For the M-B series (monomer B only), a high curing shrinkage stress led to interlayer
delamination during the stacking process, also clearly visible in Fig 2(b). In contrast, the mixed monomer formulations (M-AB series) exhibited superior flowability,
interlayer adhesion, and curing stability throughout the printing process, resulting
in the well-defined structures shown in Fig 2(c), thereby enabling the formation of structures without notable geometric distortion
or delamination. The M-AB-3 formulation achieved the highest dimensional stability
after curing, improving it by ~15% and 10% points compared to that of M-A-3 and M-B-3,
respectively [16]. Further, this can be attributed to the balanced shrinkage behavior achieved by
the mixed monomer composition, which effectively harmonizes the curing shrinkage,
viscosity, and printing quality.
Curing depth is also considered an important performance metric. Monomer A yielded
shallow curing depths with a lower shrinkage stress, which resulted in reduced warping
but insufficient layer adhesion. In contrast, monomer B cured more deeply and rapidly;
however, it induced excessive shrinkage stress, thereby leading to delamination. The
M-AB-3 formulation demonstrated an optimal balance between curing depth and shrinkage
stress, which ensures high dimensional accuracy and stable layer-by-layer stacking
behavior. Consequently, the M-AB-3 formulation, which is composed of a 1:1 weight
ratio of monomers A and B with a 3 wt% photoinitiator, was selected as the reference
resin formulation for this study. Subsequently, this formulation was used as the basis
for the further investigation of oligomer addition and optimization of ceramic solid
loading.
3.2. Effect of Oligomer Addition on Viscosity and Strength
Incorporating oligomers into photopolymerizable resin systems can enhance the mechanical
strength of cured structures and mitigate polymerization shrinkage. However, an increase
in oligomer content leads to an increase in slurry viscosity, which can adversely
affect printability during the layer-by-layer deposition process. In this study, the
effects of high-molecular-weight oligomer A were investigated using a series of formulations.
A base slurry composed of a 60 wt% Si3N4 ceramic and monomer A was prepared, and oligomer A was added at concentrations ranging
from 0−10 wt%. Each formulation was evaluated for printability using a DLP printer
and the flexural strength of a cured green body.
The slurry without oligomer A (oli-A-0) exhibited a very low viscosity of ~5,420 cP,
which resulted in the poor adhesion of the cured layer to the build platform and led
to print failure because of outflow. Similarly, the 2 wt% formulation (oli-A-2) failed
to print consistently, which was attributed to insufficient viscosity, preventing
stable layer formation. In contrast, formulations with oligomer A concentrations of
4 wt% or higher were printable, and the flexural strength of cured specimens increased
with an increasing oligomer content [17]. The flexural strength was measured to be 38, 96, and 122 MPa for oli-A-4, oli-A-6,
and oli-A-8, respectively. However, a decline in strength was observed at 10 wt% (oli-A-10),
dropping to 83 MPa. This reduction can be attributed to a decrease in the internal
bonding strength within the cured structure caused by excessive oligomer content or
reduced light penetration and non-uniform curing resulting from increased viscosity
[17]. The viscosity showed a near-linear increase with oligomer content, which reached
~9,100 cP at 8 wt% oligomer A (Table 2).
Additional experiments were conducted by partially substituting the low-viscosity
oligomer B to address the issue of increased viscosity associated with oligomer A.
The total oligomer content was fixed at 8 wt%, and six formulations (oli-AB-0 to oli-AB-10)
with varying A:B ratios were prepared. The viscosity and flexural strength of the
cured structures were evaluated for each formulation. The results demonstrated a consistent
decrease in viscosity with increasing B content, while the flexural strength increased
to a maximum and then declined. The A:B = 4:4 formulation (oli-AB-8) exhibited the
most favorable performance with a reduced viscosity of ~7,000 cP and a maximum flexural
strength of 154 MPa [18]. This result indicates an optimal balance between polymer density and viscosity
control, thereby suggesting that oligomer B not only improves the flow characteristics
of the slurry but also contributes to the formation of a sufficiently crosslinked
network. This optimized performance is a direct consequence of both the differential
viscosities of the oligomers and the contributions of their distinct chemical functionalities
to the polymer network. High-viscosity oligomer A (4,560 cP) is a hexafunctional urethane
acrylate oligomer. Its incorporation significantly increases the crosslinking density
of the cured body, leading to higher green body strength (e.g., 122 MPa for oli-A-8)
and improved durability, albeit with a tendency towards increased brittleness due
to its high functionality. Conversely, low-viscosity oligomer B (384 cP) is a difunctional
urethane acrylate oligomer. It contributes to reducing the overall slurry viscosity
for improved processability, but more importantly, it provides a more flexible chain
structure within the crosslinked network. This flexibility effectively enhances interlayer
adhesion and mitigates the brittleness associated with oligomer A's high crosslinking
density, thereby balancing the overall mechanical performance with optimized flowability
In contrast, the formulation with 5 wt% oligomer B (oli-AB-10) exhibited the lowest
viscosity (6,480 cP) but reduced flexural strength (133 MPa) [19]. These findings suggest that an appropriate combination of high- and low-viscosity
oligomers is crucial for achieving a balance between mechanical performance and printability
in photocurable resin systems (Table 3).
Based on the optimized formulation (monomer A/B = 1:1, photoinitiator 3 wt%, oligomer
A/B = 4 wt%/4 wt%, and dispersant 4 wt%), a systematic evaluation of the ceramic solid
loading from 60-68 wt% was conducted to determine the printability threshold. Viscosity
measurements showed that slurries containing up to 66 wt% ceramic maintained a moderate
increase in viscosity, achieving a value of ~15,000 cP, which ensured stable layer
deposition. However, at 68 wt%, the viscosity exceeded 20,000 cP, thereby resulting
in difficulties in layer re-coating and material spreading [20]. These results are consistent with previous reports indicating that slurry viscosities
beyond 20,000 cP compromise layer uniformity in DLP processes. Accordingly, 66 wt.%
was established as the practical upper limit for the ceramic solid content in the
slurry.
The final slurry formulation with 66 wt% ceramic content exhibited excellent layer-wise
buildability and mechanical strength, and allowed the successful fabrication of complexshaped
test pieces and spinal cage prototypes. This demonstrates the validity of the proposed
formulation strategy for high-solid-content Si3N4-based photopolymerizable slurries for DLP-based additive manufacturing.
3.3. Optimization of Ceramic Solid Content
As summarized in Table 4, five formulations (S_62–S_70) were prepared by fixing the optimized resin composition
(monomer A/B = 1:1, photoinitiator 3 wt%, oligomer A/B = 4 wt%/4 wt%, and dispersant
in the range of 3.0–3.8 wt%) while incrementally increasing the ceramic powder content
from 62 to 70 wt% in 2 wt% intervals. The viscosity of each slurry was measured using
a rotational viscometer. The target upper limit for the slurry viscosity was set to
20,000 cP for ensuring defect-free and dimensionally accurate printing in the DLP
3D printing process.
According to the viscosity measurement results shown in Fig 3, the viscosity increased moderately from ~11,800 to 15,000 cP with an increase in
solid content from 62 to 66 wt%. However, a further increase from 66 to 68 wt% caused
a sharp increase of more than 33%, which exceeded 20,000 cP. For the formulation with
70 wt% solid content (S_70), the viscosity surpassed 30,000 cP, and during the actual
printing, frequent defects such as blade coating failure and incomplete layer filling
were observed, thereby making it difficult to achieve stable layer-by-layer printing
[21].
Ceramic solid loading affects photopolymerization depth in addition to viscosity.
The curing depths of the three formulations(S_64, S_66, and S_68) were measured to
evaluate curing behavior. The experiment was conducted by irradiating a fixed range
of energies (400–1400 mJ/cm2) using a DLP processor. The results are presented in Fig 4. The curing depth increases linearly with an increase in exposure energy. However,
for the high-solid-loading formulation S_68, the curing depth was significantly lower
than that of S_64 and S_66 under the same exposure conditions [22]. This behavior can be attributed to enhanced light scattering by the ceramic particles
in the slurry, which reduces the effective UV penetration depth, thereby limiting
the achievable curing thickness. The rate of increase in the curing depth sharply
declinedwhen the exposure energy exceeded 50 mJ/cm2, thereby approaching the saturation region. This finding indicates that maintaining
the exposure energy below 50 mJ/cm2 is more favorable to achieving stable curing. These results experimentally demonstrate
that solid loading influences not only the rheological properties but also the photopolymerization
mechanism, and it supports the conclusion that S_66 offers the most balanced performance
in terms of printability and curing behavior during the subsequent layer-by-layer
fabrication and sintering processes.
3.4. Thermal Stability Evaluation of the Slurry via TGA Analysis
Analyzing the thermal stability and decomposition behavior of the organic components
within the slurry is necessary as the photopolymerizable ceramic slurry undergoes
debinding and sintering after printing to fabricate the final structure. In this study,
TGA was conducted to investigate the decomposition characteristics of individual components
(monomers A, B, A, and B). The results are presented in Fig 5. Further, TGA was performed on the green body fabricated using the optimized slurry
to evaluate the thermal decomposition behaviors of the binders. As discussed in the
experimental procedure, the TGA curve showed a total weight loss of ~16 wt% up to
400 °C, after which little to no further change occurred. This implies that most of
the organic components, including monomers, oligomers, and dispersants, were thermally
decomposed below 400 °C [23]. The initial steep weight loss near 120 °C is attributed to the evaporation of low-molecular-weight
monomers, while the gradual loss between 150 and 400 °C corresponds to the thermal
decomposition of oligomers.
Based on these findings, the debinding process was designed to heat the green body
up to 400 °C. After thermal treatment at this temperature, the residual weight of
the sample was ~83.5 wt%, which corresponds to the combined weight of the ceramic
powders (66 wt%) and sintering additives (Y2O3 + Al2O3, 9.9 wt%), thereby confirming the complete removal of organics. The debound specimen
retained its shape without any visible shrinkage or cracks, which suggests that the
internal stress caused by porosity during decomposition was minimized [24].
Beyond 400 °C, negligible weight changes were observed for all resin components, which
indicate that the major organic species were completely decomposed at this temperature.
Accordingly, the optimal temperature for the debinding process for removing organic
constituents in the slurry was established to be ~400 °C. The formation of residual
pores in the final sintered body was expected to be minimized by applying a debinding
profile based on the temperatures that completely remove the monomers and oligomers.
3.5. Evaluation of the Mechanical Properties of the Sintered Bodies
X-ray diffraction (XRD) analysis of the sintered specimens confirmed the successful
phase transformation from α-Si3N4 to the desired β-Si3N4 phase after sintering, as presented in Fig 10. This verifies the Si3N4 ceramic had the proper intended formation.
Under sintering conditions at temperatures above 1800 °C all of the compositions (S_64,
S_66, and S_68) achieved a relative density exceeding 99% (Fig 6(a)). It was observed that with an increase in solids loading densification began at
lower sintering temperatures. Furthermore, the S_64 composition, with its lower solid
content and density, exhibited clustered pores and defects, as clearly seen in its
microstructure (Fig 6(b)). In contrast, the S_66 composition (Fig 6(c)) showed a significantly denser microstructure with reduced porosity. The S_68 composition,
having the highest solid loading, achieved the highest relative density, and its microstructure
(Fig 6(d)) consistently showed minimal bulk porosity, indicative of highly effective densification.
The overall trend of decreasing bulk porosity and increasing densification with higher
solid content is clearly depicted across the microstructures presented in Fig 6(b-d). An increase in density with higher sintering temperatures is one of the commonly
observed characteristics in ceramics [25]. However, despite excellent bulk density, issues such as layer delamination were
observed during printing, which subsequently affected its three-point flexural strength.
The mechanical strengths of the sintered bodies were evaluated using a three-point
bending test on specimens with dimensions of 4 × 3 × 35 mm. The specimens were fabricated
in both horizontal (laid on the X-Y plane) and vertical (standing on the X-Y plane)
build orientations (Fig 7), and ten specimens were tested for each condition to determine the average and standard
deviation. The results confirmed that the flexural strength increased with higher
sintering temperatures across all compositions, with S_66 exhibiting the highest strength
at 1800 °C (Fig 8) [26]. However, the high solid loading composition S_68 showed a significant reduction
in strength of ~30–40% in the vertically printed specimens, which was attributed to
interlayer bonding defects and layer delamination, which were directly observed during
the printing process and post-printing inspection. Representative SEM images (Fig 9) clearly illustrate these interlayer bonding defects and delamination phenomena in
the vertically printed S_68 specimens, particularly at high solid loadings where slurry
flowability and uniform layer spreading are hindered, resulting in poor print quality.
Vickers hardness measurements were conducted under a load of 4.9 N (500 gf) using
a Vickers hardness tester. All of the compositions exhibited hardness values exceeding
1500 HV when sintered above 1750 °C, with S_66 demonstrating consistent hardness stability
across the entire temperature range. The fracture toughness was calculated based on
crack lengths emanating from Vickers indentations using the indentation fracture (IF)
method. The results confirmed a gradual increase in fracture toughness with sintering
temperature, followed by a sudden decrease at 1850 °C. This decrease was attributed
to excessive grain growth during oversintering, which increased the brittleness of
the ceramic body (Fig 9). The comprehensive optimization process, from initial resin formulation to ceramic
solid loading, and the resultant key performance indicators of the developed Si3N4 slurry are summarized in Table 5.
4. CONCLUSION
In this study, a high solid-loading Si₃N₄ ceramic slurry suitable for DLP-based photocurable
3D printing was developed, and its formulation was optimized to ensure rheological
stability, high dimensional precision during printing, and sintered bodies with excellent
mechanical properties. The main conclusions are as follows:
1. The optimal monomer formulation was achieved by blending monofunctional monomer
A and difunctional monomer B in a 1:1 weight ratio and adding a 3 wt% photoinitiator.
The M-AB-3 composition exhibited the most favorable balance between viscosity stability
and polymerization shrinkage. In contrast, the A-only formulation showed both an increase
in viscosity over time and warping, while the B-only formulation exhibited excessive
shrinkage, thereby leading to interlayer delamination.
2. The flexural strength of the cured green bodies increased to a maximum of 122 MPa
at 8 wt% when oligomer A alone was added. However, at 10 wt% or higher, a further
increase in viscosity led to reduced strength. To overcome this, a combination of
oligomer A (4 wt%) and lower-viscosity oligomer B (4 wt%) was adopted, thereby resulting
in a slurry viscosity of ~7,000 cP and a flexural strength of 154 MPa, which demonstrated
an effective balance between flowability and mechanical strength.
3. The dispersant BYK-110 exhibited effective dispersion at ~5 wt% relative to the
ceramic content (equivalent to ~3– 4 wt% of the total slurry). With this optimized
formulation, the solid loading was increased stepwise, and stable printing was possible
up to 66 wt% while the viscosity remained below 20,000 cP. Beyond 68 wt%, the slurry
exhibited an abrupt rise in viscosity, poor re-coating, and printability issues, thereby
establishing 66 wt% as the upper solid loading limit.
4. The optimized slurry enabled stable and high-precision DLP 3D printing. Following
post-curing and mild debinding at 400 °C, pressure-assisted sintering at 1800 °C under
1 MPa of nitrogen produced sintered bodies with ~98% relative density, flexural strength
of 1,070 MPa, Vickers hardness of 1,670 HV, and fracture toughness of 7.3 MPa·m1/2. Although sintering at 1900 °C yielded comparable strength, the accompanying grain
coarsening led to a significant decrease in fracture toughness, which indicates that
1800 °C is the optimal sintering temperature.
Collectively, the precise control of monomer, oligomer, photoinitiator, and dispersant
content enabled the development of a high solid-loading Si3N4 slurry with excellent printability and mechanical performance. The proposed slurry
formulation is expected to be effectively applicable to the additive manufacturing
of complex medical ceramic components such as the Si3N4 spinal cages for spinal implant applications.