2.1. Morphology and Residual Contaminant Distribution in Spent and Regenerated Graphite
Field-emission scanning electron microscopy (FE-SEM) images and energy-dispersive X-ray spectroscopy (EDS) elemental maps (
Figure 1a,(a-1)) show that spent graphite (SG) retains deposit-rich surface films with adhered particulates. In the corresponding EDS maps, oxygen, fluorine, and phosphorus signals are broadly detected across the SG surface, with Al localized in particulate-rich regions (
Figure 1(a-1)), consistent with mixed electrolyte- and binder-derived residues (P from LiPF
6-derived species and F from electrolyte-derived fluorides and polyvinylidene fluoride (PVDF) fragments) persisting within the deposit layer [
18]. Such mixed deposit chemistry provides a plausible basis for spatially nonuniform interphase re-formation. In contrast, the regenerated samples exhibit markedly reduced surface deposits and attenuated heteroatom signals in the EDS maps (
Figure 1b,c,(b-1),(c-1)), consistent with detachment of the deposit layer and re-exposure of the underlying graphite basal and edge planes.
Transition-metal signals (e.g., Ni, Co, and Mn) are spatially localized and tend to co-occur with deposited particulates rather than appearing as uniform backgrounds (
Figure 1(a-1)). This spatial colocalization suggests that most metallic impurities are present as discrete particulates or surface-attached fragments, rather than being incorporated into the graphite lattice. Such localization may contribute to spatially heterogeneous interphase formation during subsequent cycling [
19,
20]. The observed distribution is consistent with the positive-electrode-to-negative-electrode crosstalk during long-term cycling and the physical carryover of positive-electrode fragments during dismantling.
After wet chemical regeneration, the malic-acid-treated graphite (MG; obtained via acidic malic-acid leaching) and EDTA-treated graphite (EG; obtained via EDTA chelation under alkaline conditions (pH 8.7)) exhibit reduced surface deposits (
Figure 1b,c), with elemental maps dominated by carbon and diminished oxygen-rich features (
Figure 1(b-1),(c-1)). This change is consistent with the detachment of the deposit phases and re-exposure of the underlying graphite basal and edge planes. Because the basal and edge planes differ in surface reactivity and functional-group density, the extent and chemistry of this re-exposed surface are expected to influence the initial pathways of SEI re-formation during formation cycling. The smoother basal texture and sharper edge features become more evident after regeneration, approaching the surface morphology of commercial graphite (CG) (
Figure 1d).
Consistent with this morphological recovery, the heteroatom (F and P), Al, and transition-metal signals that are prominent or localized in the SG are substantially suppressed in the regenerated samples (often near the EDS-mapping sensitivity). The resulting maps are C-dominated, with only weak O contributions (
Figure 1(b-1)–(d-1)). This re-exposure of the basal and edge planes is expected to recover electrochemically accessible graphite surfaces for subsequent lithiation and delithiation. The reduced deposit phases and metal-bearing particulates may decrease the electrochemically inactive surface blockage, thereby limiting the localized sites for parasitic electrolyte decomposition [
19,
21]. The implications for interfacial resistance are discussed in
Section 2.5. These changes indicate the concurrent removal of physically and chemically distinct contaminant phases and alteration of the near-surface chemical state that governs interphase formation and impedance evolution. Next, the extent of impurity removal was quantified by ICP–MS (
Section 2.2). The chemical speciation of the residual near-surface layer is discussed later using depth-resolved XPS (
Section 2.6).
2.2. Quantitative Impurity Removal by Malic-Acid Leaching and EDTA Chelation
Inductively coupled plasma mass spectrometry (ICP–MS) shows that both malic-acid leaching (performed with glucose as a reducing agent;
Section 3.2) and EDTA chelation reduce the elemental impurity levels in SG by >99% under matched conditions (
Figure 2a). This brings the total impurity levels close to the commercial benchmark (
Figure 2 and
Table S1). SG contains a high total-impurity concentration (217.85 ppm;
Figure 2b), dominated by Ni (122.02 ppm) with additional contributions from Li, Mn, Co, and Al (
Figure 2a). This transition-metal-rich profile is consistent with the positive-electrode-derived species reaching the negative electrode during cycling or via carryover during dismantling (
Section 2.1).
After regeneration, the total impurities decrease close to the commercial benchmark (1.82 ppm for MG and 1.73 ppm for EG, versus 1.02 ppm for CG;
Figure 2b), corresponding to a >99% reduction relative to SG. For Ni and Co, concentrations decrease from 122.02 and 22.98 ppm in SG to below the detection limit for Ni and ~0.04–0.05 ppm for Co in MG/EG (
Figure 2a, inset), indicating that both approaches reduce transition-metal contaminants to sub-ppm levels. Deposited transition metals can accelerate parasitic electrolyte reactions and destabilize the interphase development [
19,
21]. Therefore, achieving sub-ppm levels can isolate the route-dependent effects of leaching-induced near-surface chemical and defect states. In this regime, transition-metal-catalyzed parasitic reactions are minimized as dominant variables, and electrochemical recovery becomes more sensitive to the leaching-conditioned surface functional groups and defect populations that govern SEI re-formation.
With the suppression of dominant transition metals, the residual impurity budget becomes more diagnostic of minor sources. In both MG and EG, P- and Fe-containing species accounted for most of the remaining sub-ppm levels (
Figure 2a, inset). This pattern is consistent with the electrolyte-salt–derived and hardware-related trace contributions becoming more apparent once the transition metals are removed. Al and Cu detected at low levels may reflect minor current collectors or casing-derived particulates introduced during recovery. The comparable post-treatment impurity levels (
Figure 2b) suggest that bulk purification is unlikely to be the main discriminating factor between the two chemistries under the same conditions. Because ICP–MS quantifies the bulk composition after digestion, near-surface residues relevant to SEI formation can differ between routes, even at comparable total-impurity levels. Instead, the remaining differences in performance may be associated with the interaction of the two leaching environments with the graphite surface during contaminant extraction.
These two regeneration environments mobilize contaminants through distinct chemical driving forces. In the malic-acid approach (pH 2.2), metal oxides/hydroxides dissolve primarily via proton-promoted weakening of M–O bonds, which increases metal-ion solubility [
22]. Carboxylate ligands can additionally stabilize the dissolved metals and further shift the dissolution equilibria. In the EDTA route (pH 8.7), extraction proceeds mainly by chelation; stable metal–EDTA complexes lower the activity of dissolved ions and sustain ligand-promoted dissolution under alkaline conditions [
23]. EDTA provides multidentate carboxylate and amine donor sites that remain effective at pH 8.7, enabling complexation-driven extraction without strong acidity. Once the total impurities are reduced to ~1–2 ppm by either route (
Figure 2b), the remaining differences in the electrochemical recovery are more plausibly governed by the surface and defect states generated during leaching. This leaching-induced state can influence the subsequent SEI re-formation and resistance growth [
24,
25]. Accordingly,
Section 2.3 and
Section 2.6 focus on route-dependent changes in the sp
2 framework and near-surface speciations that control the interphase evolution.
2.3. Structural Ordering and Defect Evolution After Regeneration and Heat Treatment
X-ray diffraction (XRD) and Raman spectroscopy show that the acidic and alkaline wet-chemical regeneration routes impose different degrees of lattice perturbation and defect evolution (
Figure 3). Here, the suffix “-H” denotes the heat-treated counterparts of the wet-regenerated samples (1200 °C post-treatment;
Section 3.3), i.e., MG-H and EG-H are obtained by heat treating MG and EG, respectively. To distinguish the respective contributions of wet impurity removal and thermal post-treatment, MG and EG represent the materials after wet processing (before 1200 °C), while MG-H and EG-H represent the corresponding materials after the identical 1200 °C post-treatment (
Section 3.3). Accordingly, the wet-processing effect is assessed by SG → MG/EG, and the incremental heat-treatment effect is assessed by MG → MG-H and EG → EG-H. The subsequent heat treatment partially restores graphitic ordering.
In the XRD patterns (
Figure 3a), SG shows additional reflections that can be indexed to Ni and NiO alongside the graphite peaks, consistent with the high Ni level measured by ICP–MS. These impurity-related reflections are suppressed after wet processing and are no longer prominent after heat treatment, consistent with either the removal of crystalline Ni/NiO phases or a reduction below the XRD-detection limit. In the enlarged (002) region (
Figure 3b), MG shows a slightly broader and lower-angle (002) reflection than EG, suggesting greater interlayer expansion and stacking disorder after acidic leaching. The corresponding d002 values are of 3.414 and 3.404 Å for MG and EG, compared with 3.396 and 3.371 Å for SG and CG, respectively. After the heat treatment, the (002) peak sharpens and shifts toward CG. EG-H shows the closest agreement with CG (d002 = 3.371 Å), whereas MG-H remains slightly expanded (d002 = 3.381 Å). This residual expansion suggests that some acid-conditioned lattice perturbation persists after thermal treatment. The corresponding near-surface chemical signatures are discussed in
Section 2.6. The larger (002) shift and broadening of MG are consistent with stronger lattice perturbations during acidic leaching. This may reflect the acid-promoted generation of oxygenated edge/defect sites (
Section 2.6), which may weaken interlayer cohesion. In comparison, the EDTA route (pH 8.7) shows a smaller shift, consistent with limited stacking disruption under the present conditions.
Raman spectra are commonly used to qualitatively assess defect- and edge-related disorders using the D-to-G band area ratio (A
D/A
G) [
26,
27] (
Figure 3c). The D band (~1350 cm
−1) and G band (~1580 cm
−1) are used to compute A
D/A
G. The SG exhibits the highest defect signature (A
D/A
G = 0.47). Wet-chemical regeneration decreases A
D/A
G to 0.44 (MG) and 0.38 (EG), consistent with a reduced defect- and edge-related contribution, even before heat treatment. Heat treatment further reduces A
D/A
G to 0.28 and 0.22 for MG-H and EG-H, respectively, with EG-H approaching CG (0.21). The relative magnitude of the A
D/A
G change separates deposit removal from framework recovery. The modest A
D/A
G decrease after wet processing (MG and EG), relative to the pronounced decrease after heat treatment, indicates that deposit removal and impurity extraction alone do not fully restore the sp
2 framework. Therefore, substantial defect healing and restacking require high-temperature treatments. A
D/A
G reflects both intrinsic structural disorder and contributions from edge-rich/disordered surface deposits; accordingly, the decrease after wet processing is attributed to deposit removal, together with the partial recovery of the underlying graphitic framework.
Consistent with the (002) behavior (
Figure 3b), the alkaline route (from EG to EG-H) achieves a lower residual disorder after heat treatment (
Figure 3c), suggesting that minimizing the chemical perturbation during wet processing facilitates a more complete structural recovery upon heat treatment. This trend suggests that acidic leaching may introduce or preserve more defect/edge-reactive sites than alkaline chelation, whereas the high-temperature treatment promotes defect healing, restacking, and the removal of defect-associated surface functionalities [
28,
29,
30,
31]. Therefore, the structural data suggest that regeneration should be evaluated not only by impurity removal but also by how strongly the leaching environment perturbs the sp
2 framework. Defect density and edge chemistry can directly influence interphase re-formation and long-term electrochemical stability [
24,
25], consistent with the route-dependent impedance response and depth-resolved surface-chemistry trends discussed in
Section 2.5 and
Section 2.6.
2.4. Electrochemical Behavior of Regenerated Graphite in Half-Cells
Half-cell testing shows that, beyond impurity removal, the structural and near-surface states produced during regeneration can influence the polarization (overpotential) and cycling stability (
Figure 4 and
Table S2). SG shows limited reversible capacity and rapid fading, consistent with residual contaminants and a reactive, inhomogeneous surface that can sustain parasitic reactions and unstable interphase growth [
32] (
Figure 4a,c). In
Figure 4a, SG reaches the upper cutoff voltage at a markedly lower capacity and shows a wider charge–discharge voltage hysteresis than the regenerated samples, indicating stronger polarization (larger lithiation/delithiation overpotential). The cyclic voltammograms show lower peak currents, broader lithiation/delithiation features, and an anodic peak shifted to higher potentials for SG (
Figure 4b), consistent with slow interfacial kinetics. In contrast, the regenerated samples exhibit stronger and sharper redox features, and EG-H approaches CG (
Figure 4a,b), suggesting the partial recovery of reversible interfacial kinetics. Regenerated samples recover capacity to near-commercial levels at early cycles: the initial discharge capacities are 350 (MG) and 346 mAh g
−1 (EG), compared with 365 mAh g
−1 for CG (0.1 C) (
Figure 4a and
Table S2). After heat treatment, the initial discharge capacities reach 362 (MG-H) and 365 mAh g
−1 (EG-H). The initial Coulombic efficiencies also improve from 89% (SG) to 90% (MG/EG) and 92% (CG/MG-H/EG-H), which is consistent with the reduced irreversible Li consumption during the initial interphase formation [
33].
Despite similar initial capacities, the cycling stability differentiates the routes. After 100 cycles, the capacity retention increases from 33% (SG) to 47% (MG) and 68% (EG), and further to 70% (MG-H) and 87% (EG-H), comparable to that of CG (87%) (
Figure 4c and
Table S2). The rate capability further supports a polarization-limited response at high current densities: the discharge capacity decreases sharply at 1–10 C but largely recovers when the rate returns to 0.1 C (
Figure 4d). This recovery indicates that the high-rate losses are largely reversible and dominated by polarization rather than by irreversible capacity loss. Within this polarization-limited regime, MG delivers higher discharge capacities at intermediate rates (1–5 C) than EG. Conversely, EG shows higher capacity retention during 1 C cycling (
Figure 4c), highlighting a rate–lifetime trade-off between the two wet-chemical routes. This divergence indicates that the wet-processing environment can decouple short-term interfacial transport (rate capability) from long-term interphase passivation (capacity retention) once bulk impurities are largely suppressed.
This contrast is consistent with the malic-acid route yielding a leaching-conditioned near-surface state that is comparatively favorable for Li
+ transport at elevated rates, but less passivating over extended cycling. In contrast, alkaline chelation combined with a heat treatment tends to suppress defect-driven side reactions that promote continued interphase growth. The separation between MG and EG, and between MG-H and EG-H, is observed even though bulk impurity levels are already comparable by ICP–MS. These trends are consistent with a surface-controlled mechanism once bulk contaminants are suppressed as a dominant variable. This interpretation is further supported by the EIS analysis (
Section 2.5) and the depth-resolved XPS results (
Section 2.6), which are discussed in the following subsections. Acidic processing may leave a more defect-rich and oxygenated near-surface region, thereby facilitating continued SEI growth and increasing the impedance during cycling [
24,
25]. In contrast, alkaline chelation tends to preserve structural integrity and yields a near-surface state that is more favorable for stable SEI re-formation after a heat treatment. Therefore, the electrochemical data indicate that regeneration routes should be evaluated based on the structure and near-surface state, as well as purification, because the dominant degradation mode can shift to interphase-controlled loss once transition-metal contaminants are largely removed [
34,
35].
2.5. Interfacial Resistance and Kinetic Parameters from Electrochemical Impedance Spectroscopy
EIS Nyquist plots (
Figure 5a) exhibit a high-frequency semicircle and low-frequency diffusion tail. The spectra are collected after the formation cycling and are stabilized at 0.7 V (
Section 3.5); therefore, the fitted parameters primarily reflect the nascent interphase formed on each regenerated surface. The spectra are fitted using the equivalent circuit R
S–(R
SEI‖CPE
SEI)–(R
CT‖CPE
CT)–W
O (
Figure 5c) [
36,
37]. In this circuit, “‖” denotes a parallel combination. R
S represents the uncompensated ohmic resistance (electrolyte, separator, and contact contributions), R
SEI the SEI resistance, and R
CT the charge-transfer resistance. CPE
SEI and CPE
CT are constant phase elements that describe the nonideal capacitive behavior, and W
O is the Warburg element capturing the diffusion-related response.
Table 1 summarizes R
SEI, R
CT, and their sum (R
SEI + R
CT). Because porous/heterogeneous composite electrodes typically exhibit depressed semicircles (i.e., nonideal capacitive response), CPE terms are used here to capture the distribution of relaxation times and to obtain stable fits. Accordingly, the extracted resistances should be regarded as effective (model-dependent) parameters, and the discussion focuses on trends that are also apparent from the raw Nyquist semicircle sizes (
Figure 5a,b) and from the total interfacial resistance (R
SEI + R
CT) summarized in
Table 1.
The fitted parameters quantify the effect of regeneration on these contributions. SG exhibits the largest impedance response, with an enlarged semicircle and extended low-frequency tail (
Figure 5a), indicating large SEI and charge-transfer resistances. SG consistently shows the highest fitted R
SEI and R
CT values (
Table 1). Both wet-chemical routes reduce these resistances, and the heat treatment yields the responses closest to the commercial benchmark, as highlighted by the enlarged low-impedance view (
Figure 5b). The SEI resistance (R
SEI) decreases from 46.7 Ω (SG) to 12.4 Ω (MG) and 24.8 Ω (EG), and further to 7.8 Ω (MG-H) and 6.4 Ω (EG-H), compared with 5.7 Ω for CG. A parallel trend is observed for the charge-transfer resistance (R
CT) (33.2, 19.8, 23.1, 2.9, 3.7, and 1.8 Ω for SG, MG, EG, MG-H, EG-H, and CG, respectively). The fitted R
SEI + R
CT follows the same order (79.9, 32.2, 47.9, 10.7, 10.1, and 7.5 Ω for SG, MG, EG, MG-H, EG-H, and CG, respectively). Notably, MG-H and EG-H exhibit very similar low resistances close to CG; therefore, their small numerical difference at the measurement point (0.7 V) is treated as comparable within fitting uncertainty and does not affect the main conclusions.
The fitted parameters show that the heat treatment substantially reduces the interfacial resistance, aligning with an interphase formed in a less reactive and better-ordered near-surface state. This interpretation is supported by the heat-treatment-driven decrease in the oxygenated carbon contributions and accompanying shift in the SEI-relevant near-surface speciation observed by depth-resolved XPS (
Section 2.6). The extracted resistances are effective parameters within the chosen circuit, and are used to compare samples measured under identical conditions.
In addition, although MG exhibits a lower R
SEI than EG at the measurement point (
Table 1), EG exhibits a higher long-term retention, indicating that early-stage impedance does not fully capture the subsequent interphase evolution [
38]. This comparison suggests that a slightly more resistive initial film can be more passivating, thereby suppressing continued electrolyte decomposition and limiting the deleterious interphase growth during cycling [
39,
40]. Accordingly, the impedance trends are interpreted in conjunction with the depth-resolved XPS results to relate the resistance behavior to near-surface speciation, which biases SEI formation and its evolution during cycling.
2.6. Depth-Resolved Surface Chemistry and SEI-Relevant Species
XPS depth profiling links the regeneration environment to the SEI-relevant near-surface speciation [
41,
42]. The depth profiles are acquired from the electrodes harvested after the third formation cycle. Therefore, the profiles reflect the nascent SEI on each regenerated graphite surface. Here, ‘etching time’ refers to the cumulative Ar+ sputter-etching duration used for XPS depth profiling (0–720 s) (
Figure 6 and
Figure 7). The quantified relative fractions summarized in
Figure 6 and
Figure 7 are obtained from the peak deconvolution of the corresponding high-resolution spectra; representative peak-fitting results are provided in
Figure S1 (MG and EG) and
Figure S2 (MG-H and EG-H). Sputter yields depend on the matrix and Ar+ sputtering can perturb labile interphase components; therefore, the etching time is used as a relative depth coordinate. The profiles are discussed primarily as relative trends under identical sputtering conditions.
Clear route-dependent trends emerge in the C 1s-derived speciation under identical sputtering conditions. MG exhibits a more oxygenated outermost layer, where the graphite component is 28% and the C=O content reaches 49% at an etching time of 0 s (
Figure 6a). In contrast, EG exhibits a higher graphite fraction (32%) and lower C=O fraction (38%) at 0 s (
Figure 6b). The heat treatment increases the graphite contribution at the outermost surface for both routes: MG-H reaches 40% graphite and 24% C=O at 0 s (
Figure 6c), whereas EG-H reaches 49% graphite and 22% C=O (
Figure 6d). As the etching time increases, the graphite fraction increases in all cases (e.g., from 28% to 42% for MG and from 49% to 56% for EG-H;
Figure 6a,d), indicating that an oxygen-containing layer is concentrated near the surface where SEI formation is initiated [
42,
43,
44]. For EG-H, C=O remains in a narrow range (~22–24%), whereas COOH and “Other” decrease with etching time (
Figure 6d). A similar decrease is observed for MG-H (COOH: 17% at 0 s → 10% at 720 s;
Figure 6c), indicating that the O–C=O (COO−/COOH) contribution is concentrated near the outermost surface and is progressively attenuated as the graphite signal becomes dominant with etching time. Thus, the total oxygenated fraction decreases overall despite the relatively stable C=O contribution. Within the XPS-information depth, a lower graphite fraction at 0 s reflects stronger attenuation by an oxygenated overlayer (e.g., SEI or residual surface species), whereas a higher graphite fraction suggests a thinner or less oxygen-rich near-surface layer. This interpretation is consistent with the improved initial Coulombic efficiencies after heat treatment (
Section 2.4), suggesting reduced irreversible Li consumption during formation.
Li-containing speciation further differentiates the routes (
Figure 7). MG exhibits a substantial LiOH contribution at the outermost surface (16% at 0 s), which decreases with increasing etching time (8% at 720 s) (
Figure 7a). The elevated LiOH fraction at the outermost surface is consistent with the more reactive near-surface chemistry, indicating that the nascent interphase is less carbonate-dominated in the early stages. LiOH has been reported to promote a compositional transformation of organic SEI components, where lithium ethylene di-carbonate (LEDC) is converted to lithium ethylene mono-carbonate (LEMC) with concomitant Li
2CO
3 formation (LEDC + LiOH → LEMC + Li
2CO
3) [
45]. Because LEMC is relatively soluble, this transformation can fragment or partially dissolve the initial SEI, increasing electrolyte access to fresh graphite surface and thereby promoting continuous SEI re-formation. By contrast, EG exhibits a Li
2CO
3-dominated profile (83% at 0 s), whereas LiOH accounts for 7% at 0 s and remains as a minor component (
Figure 7b). A carbonate-dominated (Li
2CO
3-rich) interphase with low LiOH is therefore expected to be more passivating and less prone to dissolution-driven re-formation, consistent with the more stable interfacial behavior observed for the alkaline route. After heat treatment, the LiOH fraction decreases in MG-H and remains low in EG-H (
Figure 7c,d), whereas the carbonate-dominated compositions persist. ROCO
2Li and the apparent Li
2O contribution become more evident at longer etching times, particularly after heat treatment. Notably,
Figure 7 is normalized within the Li-containing speciation set, whereas the COOH (O–C=O/COO−) fraction in
Figure 6 is normalized to the total C 1s signal; therefore, the ROCO
2Li trend does not need to mirror the COOH depth trend. Ar+ sputtering can modify fragile SEI components; therefore, the Li
2O trend is interpreted conservatively as a depth-dependent increase in the more inorganic inner-layer signal, rather than as a strictly quantitative thickness-resolved phase map. However, the consistent increase in the inorganic fraction with etching time is compatible with a carbonate-rich outer region and a more inorganic inner region within the nascent interphase.
These compositional differences provide a chemical basis for the electrochemical hierarchy. The oxygenated carbon functionalities and LiOH-rich species indicate a more reactive near-surface environment. Such a surface can promote electrolyte decomposition and destabilize organic carbonate-derived interphase components, favoring continued SEI growth [
45]. In particular, LiOH can drive the LEDC → LEMC transformation and associated SEI destabilization, which leads to repeated electrolyte–electrode contact and incessant SEI dissolution/re-formation [
45]. This continuous re-formation pathway provides a mechanistic basis for the progressive impedance growth and irreversible Li consumption observed during cycling when the outermost surface is LiOH-rich. Together, these features provide a plausible pathway for the continued irreversible Li consumption and progressive impedance growth during cycling. This interpretation is consistent with the higher density of polar defect/edge sites [
10,
24,
25]. These sites can shift the interphase reactions away from the carbonate-dominated compositions during formation and contribute to the increase in resistance during cycling. By contrast, a more graphitic and carbonate-rich near-surface composition is associated with lower interfacial resistance and more stable cycling, particularly after heat treatment [
46]. The depth-resolved analysis suggests that regeneration effectively conditions the surface state prior to formation, thereby biasing the subsequent SEI chemistry and evolution. Once bulk impurities are minimized to near-commercial levels, the electrochemical recovery becomes more sensitive to the chemical state and defect structure in the outermost near-surface region. These features can influence SEI re-formation and impedance evolution. More broadly, stable ion-conducting interphases and interface/interphase regulation are widely recognized as key determinants of long-term stability across rechargeable battery chemistries [
47,
48].