Interface-driven energy-independent charge extraction in GaN photocatalysts

Domain: chemistry
Published: 2026-02-18
Editorial outcome: minor_revision

Abstract
Ultrafast charge transfer dynamics are key to photocatalytic efficiency, governing energy relaxation and surface reactivity. However, the temporal evolution of carrier energy landscapes following photoexcitation, particularly at complex metal/semiconductor interfaces, remains poorly understood. Here, we present a surface- and energy-resolved investigation of ultrafast electron dynamics across bare and Pt-modified gallium nitride (GaN) surfaces using time-resolved two-photon photoemission spectroscopy. We show that photogenerated electrons rapidly thermalize to the conduction band minimum and undergo sub-picosecond trapping in nitrogen-vacancy-related surface states. Surface modification with Pt suppresses these trapping channels and introduces an energy-independent ultrafast electron transfer pathway (~50 fs) from GaN into Pt. By disentangling interfacial charge transfer from intrinsic relaxation mechanisms through tailored pump-probe configurations, we demonstrate that Pt facilitates picosecond-scale electron transport from the bulk to the surface by photoinduced dynamic band flattening. Modulating these ultrafast dynamics through interfacial engineering significantly enhances charge separation and photoelectrochemical performance. This study deepens the understanding of interface-dependent relaxation and transfer processes of photocarriers and provides valuable guidance for rational design of advanced photocatalytic systems.

Introduction
Solar-to-chemical energy conversion offers a promising pathway towards sustainable fuel production and long-term energy security1–3. Central to advancing semiconductor-based artificial photosynthesis is the ability to understand and control the dynamics of photoexcited charge carriers4,5. These carriers undergo rapid energy relaxation, trapping, and transport on ultrafast timescales before reaching reactive sites, where they drive chemical transformations on slower millisecond timescales6. Importantly, the energy relaxation dynamics of these nonequilibrium carriers strongly influence their chemical reactivity, as only carriers exceeding specific energy thresholds can overcome activation barriers associated with key redox reactions2,7. For example, photogenerated electrons with energies above 0 eV vs. RHE are required for hydrogen evolution, while photogenerated holes with energies exceeding 1.23 eV vs. RHE at pH 0 are necessary for water oxidation in water splitting1. Although significant progress has been made in understanding photo-induced charge transfer dynamics through time-resolved spectroscopy6,8–11, most studies have focused on bulk carrier behaviors or averaged interfacial processes, whereas the femtosecond energy relaxation pathways at metal/semiconductor interfaces remain poorly understood. In particular, it is not well established how surface modifications alter the initial energy distribution, defect trapping, and interfacial injection of hot carriers immediately after photoexcitation. This knowledge gap is critical because only carriers that retain sufficient excess energy on ultrafast timescales can efficiently participate in catalytic reactions. Addressing this gap is essential for guiding the rational design of photocatalytic systems capable of preserving hot carrier energy long enough to couple effectively with surface reactions.

Gallium nitride (GaN) has emerged as a compelling platform for solar fuel production, as demonstrated by previous studies on photoelectrochemical (PEC) water splitting12–14, CO2 reduction15,16, and ammonia decomposition17. The separation and transport of photogenerated carriers in GaN are intrinsically influenced by factors such as the bulk electronic structure, crystal facet orientation, morphology, and surface states18–20. Surface modification of GaN with metal cocatalysts such as platinum (Pt)14 or cobalt (Co)21 has been shown to dramatically enhance PEC performance. These hybrid catalysts benefit from engineered metal/semiconductor interfaces that optimize interactions between catalytic sites and reaction intermediates, reduce kinetic barriers, and improve charge separation. Despite these advances, the mechanistic details of how such metal/semiconductor interfaces reshape the ultrafast carrier energy landscape remain elusive. Specifically, the formation of a metal/semiconductor junction introduces interfacial states14,22 that modulate the built-in electric field and band alignment23,24, thereby influencing the carrier energy landscape and transport behavior. Yet these effects have rarely been studied with sufficient energy and time resolution to capture energy-resolved ultrafast charge dynamics.

Herein, we employ time-resolved two-photon photoemission (tr-2PPE) spectroscopy to directly probe the energy-resolved femtosecond dynamics of hot electrons at bare and Pt-modified n-GaN surfaces. Our measurements reveal ultrafast thermalization of hot electrons to the conduction band minimum (CBM), followed by rapid trapping into deep-defect states near the Fermi level (EF) on sub-picosecond timescales, leading to long-lived states. Upon Pt modification, we observe a significant suppression of these defect-mediated processes, alongside the emergence of an ultrafast charge transfer pathway characterized by energy-independent electron injection into Pt within ~50 fs. By combining one-color and two-color excitation schemes, we disentangle the competing contributions of surface trapping, interfacial charge transfer, and bulk-to-surface transport under tunable excitation conditions. We find that Pt decoration enhances bulk-to-surface electron transport in the conduction band, facilitated by ultrafast interfacial electron injection and dynamic flattening of the surface band bending. The dynamic interplay of these effects promotes charge separation, significantly boosting the photoelectrochemical hydrogen evolution efficiency. Our results provide direct mechanistic insight into how interface engineering preserves hot carrier energy and enhances bulk-to-surface transport, offering a framework for rational design of cocatalysts and semiconductor interfaces to improve photocatalytic efficiency.

Results
tr-2PPE characterization of GaN photocatalyst
Figure 1a illustrates the experimental setup for time-resolved two-photon photoemission (tr-2PPE) spectroscopy used to investigate ultrafast electron dynamics in both temporal and energy domains. In this technique, a pump pulse excites electrons to generate a population of excited states, while a time-delayed probe pulse photoemits these electrons above the vacuum level. The resulting photoelectrons are energy-analyzed using a time-of-flight (TOF) detector.

Our tr-2PPE setup incorporates two ultrafast ultraviolet (UV, 4.49 eV) laser pulses and one visible (Vis, 2.58 eV) laser pulse, with their relative delay precisely controlled by two variable delay stages. The distinct photon energies enable two complementary pump-probe configurations to achieve state-resolved photoexcitation. In the one-color (UV-UV pump-probe) scheme, photoemission arises from band-to-band transitions in bulk GaN (bandgap: 3.4 eV) and from transitions involving (occupied) surface states. In contrast, the two-color (Vis-UV pump-probe) configuration enables selective probing of electron populations associated with surface defect states distributed within the bandgap (see “Methods” for further details). These configurations provide rich spectral access to nonequilibrium carrier distributions under tunable excitation conditions, as illustrated below.

The inset in Fig. 1a depicts the energy band structure of the n-GaN surface with low Mg doping concentration, which was cleaned through three cycles of Ar+ sputtering followed by annealing at 850°C in ultrahigh vacuum. This process resulted in a well-ordered (1×1) surface reconstruction, as confirmed by low-energy electron diffraction (Supplementary Fig. 1), and produced an atomically flat surface (Supplementary Fig. 2). Note that although Mg is an acceptor-type dopant, the GaN remains n-type due to the high activation energy of Mg acceptors and the low doping concentration used here. Ultraviolet photoelectron spectroscopy (UPS) measurements indicate that the valence band maximum (VBM) is located 2.51 eV below the Fermi level (EF) (Supplementary Fig. 3), consistent with previous reports on Mg-doped n-type GaN surfaces25. Raman spectroscopy identifies a high-frequency longitudinal optical phonon-plasmon coupled (LOPC) mode at 748 cm-1 (Supplementary Fig. 4), indicating n-type conductivity as the concentration of Mg acceptors is not high enough to induce effective p-type behavior26. This is further corroborated by the observation of a positive surface photovoltage response under bandgap excitation (Supplementary Fig. 5), which is characteristic of n-type surfaces. In addition, UPS spectra reveal a continuous filled electronic band arising from near-surface states extending from the VBM up to EF (Supplementary Fig. 3b), leading to an upward band bending.

We first investigated the photoelectron dynamics under one-color UV-UV excitation conditions. In this configuration, both the pump and probe pulses possess the same photon energy, with the pump pulse set to half the power of the probe at positive time delays. The fluence of the UV pump pulse was carefully controlled to a low value (~4 µJ/cm2), corresponding to an excitation density of 2×1017 cm3, thereby avoiding complications from multiple photon excitation and Auger recombination27. Figure 1b presents a pseudo-color plot of the tr-2PPE spectra of bare GaN after subtracting the background signal measured at −5 ps (the raw data is shown in Supplementary Fig. 6). The energy scale is referenced to EF to facilitate visualization of the excited-state energy distribution. The spectra reveal asymmetric and short-lived photoemission feature extending up to 3.5 eV above EF, along with a lower-energy component around EF that exhibits a significantly longer lifetime. At a delay time of 0 ps (Fig. 1c), a pronounced photoemission peak is observed near 0.06 eV above EF, accompanied by a weaker but discernible broad spectral features spanning the higher energy range (0.5 eV ≤ E−EF ≤ 3.5 eV, see inset of Fig. 1c). Given the wide bandgap of GaN (3.4 eV) and the measured surface work function of 4.19 eV (Supplementary Fig. 3a), this broad continuum is attributed to two-photon photoemission from occupied surface states lying below EF (Supplementary Fig. 7), in agreement with the UPS results. The pronounced low-energy peak is assigned to defect-related surface states near EF, populated via photoexcitation from the GaN valence band. These defect states are likely associated with interstitial magnesium (Mgi), which forms readily at low Mg doping levels due to incomplete incorporation on Ga sites28. These Mgi species can act as donor-like traps, introducing occupied electronic states below EF. Notably, as the delay time increases, this peak shifts by 85 meV towards lower energies, falling below EF, which corresponds to the equilibrium distribution of occupied states. Moreover, the peak intensity initially decreases within the first 0.05 ps, followed by a gradual rise at longer delay times. The subsequent discussion will elaborate on this behavior, attributing the peak shift to the photoexcitation dynamics associated with surface photovoltage (SPV).

Ultrafast dynamics of defect-assisted charge transfer and SPV
To resolve the temporal evolution of excited states, Fig. 2a presents representative time-resolved 2PPE traces at four characteristic energies: 2.5 eV, 1.0 eV, 0.5 eV, and −0.2 eV, corresponding to photoemission from the conduction band (CB), conduction band minimum (CBM), defect band (DB), and below EF induced by peak shift (PS), respectively. Each trace represents the integrated photoemission intensity within ±0.2 eV around the specified energy. The transient responses exhibit distinctly different dynamics across these energies. At 2.5 eV, excited electrons in the CB undergo rapid thermalization, characterized by a decay constant of 0.07 ps (see “Methods” for fitting details), leading to fast energy redistribution toward lower-lying CB states. At the CBM, the photoemission profile exhibits a sharp peak at time zero due to pump–probe temporal overlap, followed by a slower relaxation with a time constant of 0.12 ps, consistent with previously reported hot electron cooling dynamics in ZnO29 and InP30. This sub-picosecond decay is associated with the thermalization of hot electrons from higher CB states and ultrafast trapping by defect states within the DB.

In contrast, the transient feature at 0.5 eV is attributed to mid-gap DB states associated with nitrogen vacancies28, as further supported by electron paramagnetic resonance (EPR) spectra revealing a pronounced deep donors signal related to nitrogen vacancies (Supplementary Fig. 8). These defect-related features in GaN (see Supplementary Fig. 9a for detailed defect distributions) differ significantly from the characteristic gradual population typically observed during defect-state trapping, as observed in Cu2O31. Instead, we observe a pronounced and sharp emission peak with a temporal width comparable to the autocorrelation (AC) trace of pump-probe pulses, followed by a slower decay with a characteristic lifetime of 0.38 ps. These observations indicate that photoemission from the DB states proceeds via a sequential one-photon-driven excitation pathway involving a real populated intermediate state, rather than a virtual intermediate state with negligible lifetime32. This provides direct evidence for ultrafast electron trapping into deeper-lying defect levels near EF, as indicated by the time-dependent increase in photoemission intensity at this energy (Fig. 1b). Moreover, the observed fluence independence of this slower decay process further supports the assignment to an ultrafast defect capture mechanism (Supplementary Fig. 9b–d)33.

Interestingly, the dynamics at −0.2 eV relative to EF exhibit an initial intensity dip (Fig. 2a), followed by a rapid rise (~33 fs) comparable to the pump-probe AC width (~40 fs), and then a gradual increase towards saturation over 2.28 ps. This behavior suggests the emergence of electronic states below EF induced by photoexcitation. Given the low exciton binding energy in GaN (~23 meV)34, exciton formation is unlikely under ambient conditions. Moreover, the fluence-dependent measurements reveal a more pronounced ultrafast energy shift of this feature at higher excitation densities (Fig. 2b), further ruling out an excitonic origin29. Additionally, the absence of asymmetric peak shapes or phonon-spaced replica bands (Fig. 1c) excludes the possibility of polaron formation35,36. We thus attribute the signal below EF to a photoinduced shift of pre-existing trap states near EF, driven by the SPV effect.

We performed 2PPE spectroscopy focusing on the emission peak energy under varying pump fluences. With increasing pump fluence, the peak energy initially increases and subsequently decreases (Fig. 2c), indicating the coexistence of two competing SPV mechanisms. The initial positive shift (-SPV) arises from photogenerated electron trapping in surface defect states, while the subsequent negative shift (+SPV) is attributed to interband excitation in n-type GaN, as corroborated by SPV spectroscopy (Supplementary Fig. 5a–c). This interpretation is further supported by simplified simulations (Supplementary Fig. 5d, e), which reproduce the experimentally observed band flattening and show that bandgap illumination reduces the upward band bending at the GaN surface by approximately 0.1 eV. The transient signal observed below EF arises from a transient reduction in upward surface band bending upon bandgap excitation, leading to a rigid downward shift of the energy band edge, consistent with dynamic SPV effects. This feature vanishes at lower excitation fluence (Fig. 2d), as under these conditions the SPV response is predominantly governed by defect-mediated negative signals, further supporting its assignment to photoinduced SPV.

Modulation of charge transfer dynamics through surface modification
The vectorial superposition of the two SPV components described above leads to a net reduction in the surface photovoltage. This reduces the extent of band bending near the surface, which in turn narrows the space charge region and diminishes the selectivity for extracting photogenerated carriers, ultimately limiting the efficiency of solar energy conversion37. Surface functionalization with metal nanoparticles such as Pt14,24 or Au38, presents a promising strategy to overcome this limitation. By forming metal/semiconductor contacts, these nanoparticles induce additional band bending at the interface, thereby expanding the width of the space charge region. This modulation of the internal electric field enhances charge separation by promoting directional carrier extraction and reducing recombination losses. Motivated by this approach, we fabricated Pt-decorated GaN samples (denoted as Pt/GaN) to explore how surface modification modulates the hot carrier relaxation pathways and charge transfer dynamics.

Atomic force microscopy (AFM, Fig. 3a) reveals that Pt forms uniformly distributed nanoislands on the GaN surface, with an average height of ~0.65 nm (Fig. 3b), which is smaller than the photoelectron escape depth (~4 nm) at the excitation energy (4.49 eV)39. Statistical analysis of AFM images (Supplementary Fig. 10a) reveals that Pt predominantly forms discrete nano-islands with an average height size of ~0.73 nm and a surface coverage of ~56%. The homogeneous distribution across the surface indicates that charge transfer occurs primarily through localized metal/semiconductor junctions rather than continuous metallic channels. Transmission electron microscopy (TEM, Supplementary Fig. 10b, c) images show that the Pt nanoparticles are uniformly anchored on the GaN substrate with intimate interfacial contact. Moreover, scanning transmission electron microscopy (STEM, Supplementary Fig. 10d) image reveals a sharply defined, microscopically flat, and structurally uniform Pt/GaN interface. The partial Pt coverage allows us to detect photoemission signals from Pt, GaN, and their interface. Surface modification with Pt results in an increased work function of GaN from 4.19 eV to 4.43 eV (Supplementary Fig. 10c, d). High-resolution X-ray photoelectron spectroscopy (HR-XPS) of Pt 4f (Fig. 3c) indicates the predominance of metallic Pt, along with a minor contribution from Pt2+ species, likely arising from Pt–N bonding at the Pt/GaN interface14. Moreover, the characteristic binding energies of N 1s and Ga 2p3/2 in Pt/GaN exhibit a positive shift relative to those in pristine GaN (Supplementary Fig. 11), indicative of interfacial charge redistribution and the formation of strong electronic coupling at the metal–semiconductor interface.

Figure 3d presents the background-subtracted pseudocolour 2PPE spectrum of Pt/GaN acquired under one-color configuration (4.49 eV, see raw data in Supplementary Fig. 12). At time zero, asymmetric transient photoemission appears near the Fermi level, extending up to 3.5 eV, and decays within 0.3 ps. This signal arises from two-photon absorption (Supplementary Fig. 13). Notably, unlike bare GaN, the emission associated with long-lived defect trapping is fully suppressed, indicating that Pt decoration effectively passivates surface trap states. Nevertheless, the initial spectral profile of Pt/GaN remains similar to that of bare GaN (Fig. 3e), featuring a pronounced emission peak just above EF (~0.03 eV) and a weak high-energy tail (E–EF > 1 eV). This suggests that Pt modification does not substantially alter the distribution of occupied surface states and optical transition channels. As the delay increases, no spectral shift of the emission peak is observed, likely due to suppression of electron emission below EF by vacuum states30, as evidenced by the asymmetry of the peak.

Kinetic analysis of energy-sliced 2PPE spectra (Fig. 3f) reveals identical decay dynamics across excitation energies. Clearly, the relaxation dynamics in Pt/GaN extend beyond the pump-probe autocorrelation window (shaded red curve), confirming that the observed kinetics are not limited by the instrument’s temporal resolution. Fitting the time-dependent signals (see “Methods” for details) yields a time constant of 41±13 fs (Fig. 3g). Notably, the lifetimes of excited electrons typically exhibit strong energy dependence in both semiconductors29,30,40 and metals41,42. The absence of such dependence here provides compelling evidence for a uniform ultrafast energy-independent electron transfer from GaN to Pt, occurring within 41 fs across both DB and CB states.

Photoemission signatures of enhanced bulk-to-surface electron transport
We next performed tr-2PPE measurements using a two-color configuration with a Vis pulse (2.58 eV, 480 nm) and a UV pulse (4.49 eV, 276 nm) at a 25:1 intensity ratio. In this scheme, positive delay times correspond to the Vis pulse (pump) arriving prior to the UV pulse (probe), while negative delay times represent the UV pulse (pump) arriving after the Vis pulse (probe). To account for differing probe photon energies across the delay axis, all photoemission signals are referenced to kinetic energy, as illustrated in Fig. 4a, b for the background-subtracted spectra for GaN and Pt/GaN data (raw data as shown in Supplementary Figs. 14 and 15). The background signal arises primarily from single-photon UV photoemission near EF and two-photon processes induced by the Vis pulse (Supplementary Figs. 16 and 17).

At time zero, both samples exhibit similarly strong transient emission features with dynamics exceeding the pump-probe cross-correlation responses (Supplementary Fig. 18), indicating that the photoemission arises from real intermediate states. These peaks are attributed to initial excitation of VB states induced by both UV and Vis photons, as well as occupied DB states populated via UV excitation (Supplementary Fig. 19 and Table S1). Notably, the relaxation dynamics diverge significantly at longer delay times, particularly within the low kinetic energy region (E ≤ 1.0 eV, Supplementary Fig. 18), suggesting a marked influence of Pt surface functionalization on hot-carrier behavior. Analysis of the integrated photoemission intensity within the 0.5±0.2 eV energy window (Fig. 4c) reveals a significant suppression of defect-mediated trapping processes in Pt/GaN at positive delay times. This observation, consistent with the one-color measurements, demonstrates that Pt decoration modifies the energy dissipation landscape of photoexcited electrons, efficiently redirecting them away from defect-assisted trapping towards faster interfacial charge transfer.

Interestingly, the slow carrier dynamics observed within the 0.5–1.0 eV energy window at negative delay times (Fig. 4a, b and Supplementary Fig. 18), particularly for Pt/GaN, deviate from typical behaviors in semiconductor systems29–31,43 under two-color excitation, where UV excitation typically produces a sharp spectral edge at negative delays due to its higher photon energy and the ultrafast decay of photoexcited carriers. The persistence of photoemission signals beyond this expected decay window suggests the presence of a previously unrecognized charge relaxation channel that extends charge lifetimes beyond conventional expectations.

To elucidate the origin of this unexpected behavior, we compared photoemission spectra at −0.2 ps for both GaN and Pt/GaN, with the signal intensities normalized to the corresponding UV fluence (Fig. 4d). This normalization accounts for the variations of pulse fluence on sample surfaces across measurements and enables a direct assessment of the fraction of long-lived carriers. Both samples exhibit similar spectral shapes, indicating comparable energy distributions, but the signal intensity is significantly higher in Pt/GaN, implying a greater population of long-lived carriers. These observations indicate that the delayed signal predominantly originates from GaN rather than Pt, in line with the energy-independent ultrafast electron transfer from GaN to Pt within 41 fs demonstrated above. Since surface defect trapping is suppressed in Pt/GaN, the presence of this signal at −0.2 ps in both samples suggests that it is unlikely to originate from surface-trapped electrons in GaN. We therefore attribute this long-lived component to carrier transport from the GaN bulk to the surface. Given the intrinsic upward band bending of n-type GaN, such transport likely occurs in the diffusion-limited regime, providing a direct photoemission signature of bulk-to-surface charge migration.

These results indicate that Pt decoration on the GaN surface enhances the electron population involved in bulk-to-surface transport by approximately 50% (from 18% to 27%). This suggests that Pt not only provides an efficient pathway for interfacial charge transfer but also facilitates carrier extraction from the bulk. This enhancement arises from the synergistic interaction between bulk charge transport and ultrafast interfacial charge transfer: the rapid extraction of surface electrons by Pt alleviates electron trapping and accumulation at the GaN surface, thereby facilitating continuous charge diffusion from the bulk. This process is driven by a dynamic screening effect44 and the photo-induced SPV, which transiently reduces the upward band bending upon femtosecond above-bandgap excitation43. This effect is evidenced by the progressive upward shift (~0.18 eV, dashed arrow in Fig. 4b) of the low-energy emission edge in Pt/GaN with increasing negative delay time. Notably, these observations are difficult to discern under a one-color configuration (Fig. 3d), but become evident under a two-color configuration due to the higher photon fluence and distinct emission characteristics associated with visible probing, highlighting the complementary nature of the two measurement schemes in capturing a more comprehensive picture of charge dynamics.

To elucidate the timescales governing bulk-to-surface carrier transport, we analyzed the temporal evolution of the normalized photoemission intensity within the kinetic energy of 0.9 eV ± 0.2 eV for GaN and 0.65 ± 0.20 eV for Pt/GaN, as shown in Fig. 4e. Global fitting of the time traces reveals that the charge dynamics in GaN can be well-described by a single-exponential decay convolved with a Gaussian instrument response for both positive and negative delay times. In contrast, a biexponential model is required to adequately capture the dynamics at negative delays for Pt/GaN. At positive delays, the extracted lifetime for GaN is 0.098±0.015 ps, whereas a shorter lifetime of 0.059±0.015 ps is observed for Pt/GaN, consistent with the characteristic timescale of the energy-independent ultrafast interfacial charge transfer process discussed earlier. At negative delays, the dynamics in GaN yield a surface electron relaxation time of 0.38±0.08 ps, while Pt/GaN features a fast relaxation component of 0.065±0.022 ps attributed to surface electron relaxation, and a slower component with a lifetime of 1.96±0.34 ps associated with bulk-to-surface charge transport.

To gain deeper insights into the mechanism underlying the bulk-to-surface electron transport observed at negative delay times, we investigated the fluence dependence of carrier dynamics using tr-2PPE measurements, varying the UV pump fluences while maintaining a constant visible probe fluence (Supplementary Fig. 20a, b). Remarkably, Pt/GaN exhibits a pronounced increase in the transport time constants from the bulk to the surface in Pt/GaN with increasing UV photon fluence, deviating from the typical fluence-independent relaxation behavior associated with surface electrons in GaN. The findings from both one- and two-color experiments described above consistently confirm that surface defect-mediated trapping and relaxation are effectively suppressed in Pt/GaN. Although we cannot entirely rule out the involvement of bulk defect states, their contribution is expected to be limited, as supported by the fluence-independent defect-trapping dynamics observed in pristine GaN (Supplementary Fig. 21). We therefore attribute the observed fluence-dependent signal at time zero to an ultrafast positive SPV45,46, which dynamically reduces the extent of surface band bending and facilitates enhanced transport of photogenerated electrons towards the surface. At higher excitation fluences, a higher SPV leads to a transient flattening of the surface band bending, reducing the surface potential barrier and thereby promoting electron transport from deeper regions within the bulk to the surface. Interestingly, the energy distribution of surface-arriving electrons remains largely unchanged under different excitation fluences (Supplementary Fig. 20c), suggesting that this transport proceeds via a highly coherent, collective transport mechanism that is largely unaffected by scattering events or trap-mediated thermalization.

As summarized in Supplementary Fig. 20d, we present a schematic illustrating the ultrafast charge transfer and relaxation pathways in GaN and Pt/GaN under above-bandgap excitation. In pristine GaN, photoexcited electrons with excess energy rapidly thermalize to CBM within 0.38 ps and are subsequently trapped by deep surface states, leading to long-lived charge carriers (>10 ps). Upon surface modification with Pt, photoexcited electrons, regardless of their initial energy, are transferred to Pt in an ultrafast manner, altering both their energy distribution and thermalization behavior. This interfacial charge transfer mechanism efficiently prevents electron trapping at deep defect states, which are typically recognized recombination centers6,47, thereby promoting efficient charge separation. Moreover, Pt enhances electron transport from the bulk to the surface, leading to an enhanced surface charge carrier density. These findings underscore the broader implications of Pt surface modification, which alters electron transport dynamics in a manner to enhance photocatalytic performance, where efficient charge separation and interfacial transport are essential5,22,38. Beyond the specific Pt/GaN system studied here, in which the metal and semiconductor exhibit distinct work functions, interfacial electron-transfer efficiency in GaN-based photocatalytic systems is largely dictated by a combination of cocatalyst properties. Specifically, the semiconductor/cocatalyst band alignment, the chemical nature of interfacial bonding, and the ability to passivate surface states collectively dictate the kinetics and selectivity of interfacial electron transfer48. This broader perspective helps rationalize why a wide range of cocatalysts, including noble metals, transition metals, and metal oxides, can effectively facilitate carrier extraction on GaN surfaces.

PEC hydrogen evolution performance
To understand the influence of interface-driven electron transport on steady-state photochemical reactions, we further explored a prototypical photoreduction process in a photoelectrochemical (PEC) configuration using a standard three-electrode setup under Xe lamp illumination. In this system, Pt/GaN heterostructures functioned as photocathodes, enabling the directional transfer of photogenerated electrons from GaN to the Pt surface, where the hydrogen evolution reaction (HER) occurs in a pH-neutral Na2SO4 electrolyte (Fig. 5a). While n-type GaN surfaces are typically associated with oxidation pathways, the selection of HER was also motivated by the thermodynamically favorable alignment between GaN’s CBM (−3.3 eV) and the proton reduction potential (−4.5 eV). More importantly, focusing on an electron-mediated reduction reaction enables a direct correlation between the engineered interfacial electron-transfer channels and the resulting photocatalytic performance, establishing a design principle for interface engineering in photochemical systems.

Compared to pristine GaN (Fig. 5b), the Pt/GaN photocathode exhibited a significantly improved photocathodic current for HER, with the onset potential Von shifting from 0.16 V vs. RHE to 0.91 V vs. RHE. The J–V curve of GaN displayed discernible anodic photocurrents at potentials above 0.2 V vs. RHE (Supplementary Fig. 22a), which can be attributed to an oxidation reaction occurring on the n-GaN surface. The presence of surface Pt allows the Pt/GaN photocathode to sustain photocathodic current for HER even at applied potentials exceeding 0.2 V. Photocathodic chronoamperometric (I-t) HER measurements at -0.4 V vs. RHE revealed that the photocurrent of Pt/GaN was 6.6 times higher than that of GaN photoelectrode (Fig. 5c). The Pt/GaN photocathode exhibits stable photocurrent for over 800 min under continuous illumination (Supplementary Fig. 22b), demonstrating good operational durability. Moreover, the Faradaic efficiency for H2 evolution exceeds 97% at –0.4 V vs. RHE, confirming that nearly all photogenerated electrons are consumed in the HER process. Given the well-known catalytic activity of Pt toward the HER14,49, we further assessed the charge separation efficiency (ηseparation) to clarify the role of surface Pt modification in enhancing charge separation during the photochemical reaction in a Na2SO4 electrolyte containing K3[Fe(CN)6] (see details in “Methods” and Supplementary Fig. 22c). Remarkably, the Pt/GaN photoelectrode achieved a substantially higher charge separation efficiency (~14%) compared to GaN (~4%) at the same applied potential of −0.6 V vs. RHE (Fig. 5d). Moreover, photoelectrochemical impedance spectroscopy (PEIS) was employed to analyze the charge transfer resistance at the electrode-electrolyte interface. The Nyquist plots (Fig. 5e) show that Pt/GaN exhibits markedly smaller semicircle diameters than pristine GaN, indicating more efficient interfacial charge transfer facilitated by Pt decoration. These results suggest that the synergistic improvement in bulk charge separation and interfacial charge transfer collectively contribute to improved charge separation efficiency and the observed increase in hydrogen evolution activity. The photogenerated charge separation and transport behaviors observed under UHV provide mechanistic insights relevant to the PEC performance of GaN photoelectrodes with surface modifications. Nevertheless, under realistic PEC environments, the GaN(0001) surface could potentially undergo oxidation to form GaO or GaON layers, thereby leading to stronger upward band bending and modified interfacial charge-transfer dynamics. Future studies involving controlled surface oxidation (e.g., O2 plasma treatment) and Pt/GaO(GaON)/GaN heterostructures will be valuable for elucidating the detailed interfacial charge-transfer dynamics and for bridging fundamental model investigations with practical PEC interfaces.

This work uncovers the ultrafast carrier relaxation dynamics in GaN-based photocatalysts and demonstrates how interfacial engineering via Pt modification fundamentally redefines the energetic landscape and transport behavior at the metal/semiconductor junction. By employing state-resolved tr-2PPE spectroscopy, we reveal that Pt/GaN enables ultrafast energy-independent charge injection from GaN to Pt within 50 fs and promotes bulk-to-surface electron transport by dynamically flattening the surface band bending via photoinduced surface photovoltage, effectively promoting charge separation and suppressing trap-state recombination. The interplay of these processes greatly improves charge separation and utilization, resulting in an approximately 6.6-fold enhancement in PEC-driven hydrogen evolution. By deepening our understanding of metal modification of semiconductor photoelectrodes, this work extends beyond conventional surface state suppression to include charge energy thermalization and transport dynamics at complex heterointerfaces. These insights offer a conceptual framework for the rational design of hybrid photocatalytic systems with tailored carrier pathways for efficient solar-to-chemical energy conversion.

Methods
Materials and reagents
Chemicals were used for PEC measurements: Na2SO4 (98%, Alfa Aesar), K3[Fe(CN)6] (99.5%, Sinopharm Chemical). Deionized water (18.2 MΩ cm) was produced with a Millipore Q water purification system (Sigma-Aldrich). All chemicals were used as purchased without further purification. The used GaN(0001) films (thickness: 450 nm, size: 1×1 cm2) were purchased from HeFei Crystal Technical Material Co., Ltd., China.

Sample preparation
Mg-doped GaN(0001) films with a thickness of 450 nm were epitaxially grown on sapphire substrates by hydride vapor phase epitaxy (HVPE) (HeFei Crystal Technical Material Co., Ltd, China). The GaN-coated wafers were sequentially cleaned by ultrasonic rinsing in acetone, ethanol, and deionized water for 10 minutes, followed by nitrogen drying. The samples were then mounted onto molybdenum holders and transferred into the preparation chamber of the 2PPE system under a base pressure of ~1×10-10 mbar. Surface cleaning was performed by repeated cycles of Ar+ sputtering (650 eV, 10 min) and annealing at 850°C for 30 min in an ultrahigh vacuum (UHV) chamber, yielding an atomically ordered surface as confirmed by low-energy electron diffraction (LEED).

For surface Pt modification, the cleaned GaN wafers were transferred under vacuum to an electron-beam evaporation system (base pressure ~1×10−9 mbar), where a 0.5 nm Pt film was deposited at a rate of 1 Å s-1. The Pt film thickness was monitored using a quartz crystal microbalance (QCM). Post-deposition annealing at 500°C for 1 h under UHV conditions was performed to enhance interfacial contact. The resulting surface morphology was characterized by atomic force microscopy (AFM).

Time-resolved two-photon photoemission spectroscopy (tr-2PPE)
Ultrafast energy-resolved carrier dynamics were investigated using time-resolved two-photon photoemission spectroscopy (tr-2PPE) under ultrahigh vacuum (UHV) conditions at a base pressure of ~1.0×10-10 mbar and room temperature (20.6°C). A Coherent Vitara Ti:sapphire (Ti:Sa) oscillator coupled to a RegA 9050 amplifier (pumped by a Verdi 12 laser) provided pulses centered at 800 nm with a full width at half maximum (FWHM) of ~50 fs and a pulse energy of ~10 μJ. The output beam was split, with part of the 800 nm light frequency-doubled to 400 nm in a β-barium borate (BBO) crystal, subsequently pumping two noncollinear optical parametric amplifiers (NOPAs). White-light continuum generated via sapphire disks seeded the NOPAs. One NOPA delivered visible (VIS) pulses tunable between 470–560 nm (2.64–2.21 eV), while the second NOPA output at 545 nm was frequency-doubled to generate ultraviolet (UV) pulses at 276 nm. Both VIS and UV pulses were compressed using a pair of quartz prisms to achieve ~40 fs temporal resolution at the sample. The beams overlapped at the sample surface with a spot size of ~100×100 μm2, incident at an angle of ~45° relative to the surface normal. Two neutral density filters were separately used to control the fluences of UV and VIS beams. Photoemitted electrons were collected by a time-of-flight (TOF) spectrometer positioned ~3–5 mm from the surface, offering an angular acceptance of 7.3°, an energy resolution of ~50 meV.

The UV beam was first split into two beams with an intensity ratio of 2:1 by a beam splitter before entering the UHV chamber. In the one-color configuration, the pump and probe beams possessed identical photon energies, corresponding to a super-bandgap excitation to investigate the subsequent hot carrier relaxation dynamics. At positive delay times, the weaker UV beam functioned as the pump and the stronger beam as the probe; at negative delay times, their roles were reversed. In the two-color configuration, the Vis beam served as the pump and the UV beam as the probe at positive delay times, with the roles reversed at negative delay times, enabling a sub-bandgap excitation that allowed selective probing of surface defect states at positive delay times. Auto-correlation (AC) and cross-correlation (CC) measurements of pump-probe were performed on a Cu (111) single crystal featuring an occupied surface state. The Cu surface was prepared by three cycles of Ar⁺ sputtering (650 eV, 1.5×10⁻⁵ mbar) followed by annealing at 527°C for 20 min per cycle.

The transient dynamics of energy-resolved photoelectron intensity were analyzed by fitting to a model where the temporal response S(t) is described as the convolution of a Gaussian instrument response function G(t) accounting to pump-probe pulses with one or more exponential decay functions E(t):

S(t) = G(t) ⊗ E(t) (1)

where G(t) = 1/(σ*sqrt(2*π)) * exp(-(t-t0)^2 / (2*σ^2)) represents the Gaussian instrumental resolution function with σ related to the instrument’s temporal resolution, E(t) = A*exp(-t/τ) is an exponential decay function characterized by time constant τ. For kinetic traces involving multiple relaxation processes for Pt/GaN sample at negative delay time, the total response is modeled as a sum of convoluted exponentials:

S(t) = G(t) ⊗ (Σ Ai * exp(-t/τi)) (2)

Here, Ai and τi represents the amplitude and decay time of different processes, respectively. The Gaussian width σ was independently determined from auto-correlation measurements for the one-color configuration and from cross-correlation measurements for the two-color configuration, respectively.

X-ray photoelectron spectroscopy
X-ray photoelectron spectroscopy (XPS) was performed at room temperature (20°C) using a SPECS Focus 500 monochromator coupled with a Phoibos 100 electron energy analyzer. An Al Kα X-ray source (photon energy 1486.74 eV) operated at 200–300 W was employed for excitation. Spectra were collected with a photoelectron take-off angle of 90° and a fixed angle of 54.7° between the X-ray source and the analyzer, using a pass energy of 10 eV. High-resolution core-level spectra were acquired with an energy step size of 0.05 eV and processed by applying Shirley background subtraction.

Ultraviolet photoelectron spectroscopy
Ultraviolet photoelectron spectroscopy (UPS) was utilized to determine the surface work function and to probe the valence band structure of the samples. Measurements were performed at room temperature (20°C) in a UHV chamber with a base pressure of approximately 10-10 mbar, using the same setup as for XPS characterization. Helium I (He-I) radiation (21.2 eV photon energy) generated from a discharge lamp operating at 25-35 W served as the ultraviolet excitation source. The incident beam impinged on the sample surface at an angle of 50° relative to the surface normal. To precisely identify the secondary electron cutoff, a bias voltage of −5.0 V was applied between the sample and the electron analyzer during the UPS measurements.

Low-energy electron diffraction (LEED) measurements
Following in situ surface cleaning, the sample was transferred under UHV conditions to a separate chamber for low-energy electron diffraction (LEED) analysis. The LEED measurements were carried out at room temperature (20°C) in a UHV environment with a base pressure better than 1×10-10 mbar using a SPECS ErLEED 150 system. Incident electron energy of 226 eV was used to investigate the surface crystallographic structure. Diffraction patterns were recorded on a CCD detector and analyzed to assess surface periodicity and reconstruction.

Surface photovoltage (SPV) measurements
Surface photovoltage (SPV) measurements were carried out using amplitude-modulated Kelvin Probe Force Microscopy (KPFM, Bruker Dimension Icon) under ambient conditions. A Pt/Ir-coated conductive AFM probe was employed to scan the sample surface. The lift height of the tip is 20 nm. The surface potential was recorded both in the dark and under illumination. A Xe lamp (300 W, PerfectLight Co., Ltd.) equipped with a monochromator was used as the illumination source. The SPV was obtained by calculating the difference in surface potential between the illuminated and dark states. This SPV signal reflects photoinduced changes in surface band bending and charge redistribution. To improve the signal-to-noise ratio, surface potential profiles were averaged over multiple scans. In our measurement system, a positive SPV indicates the accumulation of photogenerated holes at the surface, while a negative SPV corresponds to the transfer of photogenerated electrons to the surface.

Transmission electron microscopy (TEM) and scanning transmission electron microscopy (STEM) measurements
Transmission electron microscopy (TEM) and scanning transmission electron microscopy (STEM) measurements were carried out using a Zeiss LIBRA 200 FE microscope operated at an accelerating voltage of 200 kV. The microscope was equipped with an omega-type energy filter, which was employed to acquire zero-loss filtered bright-field images, enhancing contrast and minimizing inelastic scattering contributions. A cross-sectional sample for TEM/STEM characterization was prepared using a Zeiss Crossbeam 340 focused ion beam (FIB) system with Ga ions, allowing precise site-specific thinning to produce electron-transparent sections for high-resolution imaging.

Photoelectrochemical (PEC) measurements
The photoelectrochemical properties were evaluated using a CHI660E electrochemical workstation (CH Instruments) configured in a conventional three-electrode setup. The GaN photoelectrode served as the working electrode, with a platinum foil employed as the counter electrode and a saturated Ag/AgCl electrode used as the reference electrode. An aqueous solution of 0.5 M Na2SO4 (pH≈6.8) was utilized as the electrolyte after thorough deaeration with high-purity nitrogen gas. The solution was stored in a sealed polypropylene container at room temperature (22°C) in the dark to avoid contamination and degradation. Illumination was provided by a 300 W Xe arc lamp equipped with a long-pass optical filter (λ>420 nm) to simulate visible-light conditions. Linear sweep voltammetry (LSV) was performed to record the photocurrent density (J–V curves) over a potential range from −0.8 V to 0.8 V versus the reversible hydrogen electrode (RHE) at a scan rate of 10 mV s⁻¹. The measured potentials were converted to the RHE scale using the Nernst equation: ERHE = EAg/AgCl + 0.059×pH + 0.1976. Photoelectrochemical impedance spectroscopy (PEIS) measurements (Biologic SP-300) were conducted at −0.4 V vs. RHE over a frequency range of 0.1 Hz to 200 kHz using a 5 mV AC perturbation in 0.5 M Na2SO4 solution. All PEC measurements were performed at room temperature (25°C).

To evaluate the charge separation efficiency of the photoelectrode, we used Fe3+ as a scavenger for the photogenerated electron due to fast kinetics and measured the photocurrent generated from Fe3+ reduction (JFe3+) in a 0.5 M Na2SO4 electrolyte containing 5 mM K3[Fe(CN)6]. The charge separation efficiency of the photoelectrode can be calculated using the following equation:

ηseparation = JFe3+ / Jabs (3)

where Jabs is the theoretical photocurrent density, which is taken to be 0.78 mA/cm2 for GaN film electrodes under 1.5 AM illumination19.

Peer review rounds
[{"round": 1, "reviewer_comments": {"reviewer_1": "This manuscript investigates ultrafast charge carrier dynamics at bare and Pt-decorated GaN surfaces using time-resolved\ntwo-photon photoemission spectroscopy (tr-2PPE). The authors show that Pt deposition effectively suppresses electron\ntrapping at surface defects and enables energy-independent ultrafast charge transfer from GaN to Pt. In addition, Pt induces\ndynamic band flattening that enhances bulk-to-surface electron transport. These effects collectively improve charge\nseparation and significantly enhance photoelectrochemical hydrogen evolution performance. The work is technically sound,\nwell-structured, and experimentally thorough. It provides valuable insights into the role of co-catalysts in modulating carrier\ndynamics at semiconductor/metal interfaces. Overall, this study is a valuable and well-executed. With brief clarifications on\nsurface condition and interface behavior under realistic environments, the manuscript will offer broader impact to the\nphotoelectrochemical and photocatalysis communities.\n1. The charge carrier dynamics studied under ultrahigh vacuum conditions may not fully reflect the interfacial behavior\noccuring in aqueous environments, as represented in the PEC experiments (e.g., Fig. 5). In particular, GaN (001) thin films\ngrown on sapphire inevitably expose the polar c-plane, which is susceptible to oxidation in aqueous solution, forming GaO\nlayers that can induce stronger upward band bending. It remains unclear whether similar charge transfer dynamics and band\nflattening occur in more realistic structures such as Pt/GaO/GaN or Pt/GaON/GaN. To better simulate the actual PEC\nenvironment, future studies could consider O2 plasma treatment to form GaO or GaON termination instead of Ar sputtering,\nas it may more accurately replicate the surface chemistry of GaN in aqueous conditions. I suggest discussing the current\nlimitations of this work and outlining future research directions for GaN/cocatalyst systems, particularly through probing\ncarrier dynamics on more realistic surfaces.\n2. The interfacial electron transfer from the GaN conduction band to Pt, which has a high work function, is somewhat\nexpected. This raises an important question regarding the role of the cocatalyst’s work function in facilitating charge\nextraction. Is high work function the key requirement for efficient electron transfer? As you noted in the introduction, a variety\nof co-catalysts (noble metals, transition metals, and metal oxides) have been employed on GaN PEC and photocatalytic\nsystems. It would significantly enhance the depth of the manuscript if you could provide a more universal discussion on what\nproperties of co-catalysts (e.g., work function, band alignment, chemical affinity, defect passivation ability) are critical from a\ncharge carrier dynamics perspective.", "reviewer_2": "Here, the systematic regulation mechanism of Pt modification on the ultrafast electron dynamics of GaN surface was\nrevealed, especially the discovery of an energy-independent electron injection process of ~50 fs and the revelation of its\nsynergistic enhancement effect with bulk-surface transport. The topic is attractive to the broad readership of Nature\nCommunications. So I recommend this manuscript can be accepted after revisions. And some questions should be\naddressed as following.\n1. AFM shows that Pt exists in the form of nano-islands, but no coverage statistics or particle size distribution is provided. It is\nsuggested to supplement the statistical information to determine whether the distribution of Pt is uniform and whether it forms\ncontinuous or discrete electron transmission channels.\n2. Please add TEM/STEM imaging of the Pt/GaN interface.\n3. Fig. 3g shows that the time constants range from 0.5 eV to 2.5 eV, which are indeed very close. However, the data points\nin the higher energy region (>2.5 eV) seem to be more scattered and show a slight upward trend. Please further explain\nwhether this phenomenon is due to statistical errors or if there is indeed a slight energy dependence?\n4.In the two-dimensional pseudo-color 2PPE (Fig 4b), the enhancement of low-energy signals of Pt/GaN during negative\ndelay is attributed to “bulk phase transport”. Whether this is affected by the inter-band transitions of Pt, considering that Pt\nhas strong absorption in the UV-Vis region.\n5. Lines 146-148: The low-energy surface defect states are correlated with Mg-doped defects. Line 169: The mid-bandgap\ndefect states are directly attributed to nitrogen vacancies. However, there is a lack of direct characterization (such as EPR).\n6. The photocurrent of Pt/GaN was increased by 6.6 times (Fig. 5c), but no stability data (such as the attenuation curve under\ncontinuous illumination) was provided. Further stability tests should be conducted. The Faraday efficiency should be\nsupplemented to confirm the correspondence between H2 production and current.\n7. Is it possible to enhance the mechanistic interpretation through theoretical calculations. For example, predicting the\ndensity-of-states distribution at the Pt/GaN interface or modeling the influence of SPV on the band structure.", "reviewer_3": "Using the state-resolved tr-2PPE spectroscopy, the authors uncovers the ultrafast carrier relaxation dynamics in GaN-based\nphotocatalysts and demonstrates how interfacial engineering via Pt modification fundamentally redefines the energetic\nlandscape and transport behavior at the metal/semiconductor junction.However, the manuscript needs further revisions to\nclarify the following points:\n(1) What causes deep level defects at the Fermi level? Please provide a detailed explanation.\n(2)Does the conclusion of 'energy independent charge extraction' hold true in other materials as well, or is it only observed in\nGaN?\n(3)In the introduction section, the authors described that“Despite their impressive performance, the details of how such\nsurface modifications alter the ultrafast energy relaxation pathways of photoexcited carriers are still unclear.”The unclear\nquestion lies in which aspects, as research in this field is already very common.The author did not mention the significant\nsignificance and necessity of the research."}, "author_response": "We have thoroughly revised our manuscript in accordance with the reviewers’ comments,\nincorporated additional experimental evidence, and provide here a point-by-point response to\nall the comments.\nReviewer #1 (Remarks to the Author):\nThis manuscript investigates ultrafast charge carrier dynamics at bare and Pt-decorated GaN\nsurfaces using time-resolved two-photon photoemission spectroscopy (tr-2PPE). The authors\nshow that Pt deposition effectively suppresses electron trapping at surface defects and enables\nenergy-independent ultrafast charge transfer from GaN to Pt. In addition, Pt induces dynamic\nband flattening that enhances bulk-to-surface electron transport. These effects collectively\nimprove charge separation and significantly enhance photoelectrochemical hydrogen evolution\nperformance. The work is technically sound, well-structured, and experimentally thorough. It\nprovides valuable insights into the role of co-catalysts in modulating carrier dynamics at\nsemiconductor/metal interfaces. Overall, this study is a valuable and well-executed. With brief\nclarifications on surface condition and interface behavior under realistic environments, the\nmanuscript will offer broader impact to the photoelectrochemical and photocatalysis\ncommunities.\nResponse: We sincerely thank the reviewer for the positive and encouraging evaluation of our\nwork. We fully agree that clarifying the surface condition and the interface behavior under\nrealistic environments will further broaden the impact of this study. In the revised manuscript,\nwe have provided additional clarifications to strengthen the significance of our findings for the\nphotoelectrochemical and photocatalysis communities, as detailed below.\n1. The charge carrier dynamics studied under ultrahigh vacuum conditions may not fully reflect\nthe interfacial behavior occurring in aqueous environments, as represented in the PEC\nexperiments (e.g., Fig. 5). In particular, GaN (001) thin films grown on sapphire inevitably\nexpose the polar c-plane, which is susceptible to oxidation in aqueous solution, forming GaO\nlayers that can induce stronger upward band bending. It remains unclear whether similar charge\ntransfer dynamics and band flattening occur in more realistic structures such as Pt/GaO/GaN\nor Pt/GaON/GaN. To better simulate the actual PEC environment, future studies could consider\nO2 plasma treatment to form GaO or GaON termination instead of Ar sputtering, as it may\nmore accurately replicate the surface chemistry of GaN in aqueous conditions. I suggest\ndiscussing the current limitations of this work and outlining future research directions for\nGaN/cocatalyst systems, particularly through probing carrier dynamics on more realistic\nsurfaces.\nResponse: Thank reviewer for this insightful comment. We fully agree that photogenerated\ncharge dynamics probed under ultrahigh vacuum (UHV) conditions may not completely\nreplicate those in aqueous photoelectrochemical (PEC) environments, where GaN (0001)\nsurfaces are prone to oxidation and may form GaO or GaON layers that modify the interfacial\nelectronic structure. Such surface chemistry could indeed induce stronger upward band bending\nand alter the charge transfer dynamics compared with the UHV-prepared GaN surfaces studied\nhere.\nNevertheless, we believe that our UHV-based measurements provide indispensable\nmechanistic insights at a well-defined Pt/GaN interface. Specifically, by detecting the kinetic\nenergy of photoemitted electrons in UHV, we are able to directly resolve the temporal- and\nenergy-resolved carrier generation and transport processes. These measurements establish a\nmechanistic framework that is often inaccessible in aqueous PEC systems due to additional\ncomplexities arising from surface reactions and electrolyte interactions.\nWe also very much appreciate the reviewer’s valuable suggestion regarding O plasma\n2\ntreatment or other controlled oxidation strategies to deliberately form GaO/GaON terminations.\nWe agree that such approaches could provide an effective means to better simulate the actual\nPEC surface chemistry of GaN electrodes, and we consider this as a promising direction for\nour future investigation.\nIn line with the reviewer’s valuable feedback, we have added a dedicated discussion in the\nrevised manuscript to explicitly acknowledge these limitations and to outline such future\nresearch opportunities, as below:\n(P21) “The photogenerated charge separation and transport behaviors observed under UHV\nprovide mechanistic insights relevant to the PEC performance of GaN photoelectrodes with\nsurface modifications. Nevertheless, under realistic PEC environments, the GaN (0001) surface\ncould potentially undergo oxidation to form GaO or GaON layers, thereby leading to stronger\nupward band bending and modified interfacial charge-transfer dynamics. Future studies\ninvolving controlled surface oxidation (e.g., O plasma treatment) and Pt/GaO(GaON)/GaN\n2\nheterostructures will be valuable for elucidating the detailed interfacial charge-transfer\ndynamics and for bridging fundamental model investigations with practical PEC interfaces.”\n2. The interfacial electron transfer from the GaN conduction band to Pt, which has a high work\nfunction, is somewhat expected. This raises an important question regarding the role of the\ncocatalyst’s work function in facilitating charge extraction. Is high work function the key\nrequirement for efficient electron transfer? As you noted in the introduction, a variety of co-\ncatalysts (noble metals, transition metals, and metal oxides) have been employed on GaN PEC\nand photocatalytic systems. It would significantly enhance the depth of the manuscript if you\ncould provide a more universal discussion on what properties of co-catalysts (e.g., work\nfunction, band alignment, chemical affinity, defect passivation ability) are critical from a charge\ncarrier dynamics perspective.\nResponse: We fully agree that, while a high work function, as in the case of Pt, can\nthermodynamically facilitate electron transfer from the GaN conduction band, the efficiency\nof interfacial charge extraction is also determined by several additional factors. These include\nthe relative band alignment between the semiconductor and cocatalyst, interfacial chemical\nbonding configuration, the ability of the cocatalyst to passivate surface states, surface\nmorphology, and intrinsic catalytic activity toward interfacial reactions that play important\nroles in defining the rate and directionality of carrier transfer.\nConsidering these aspects, we have now expanded the discussion in the revised manuscript to\nprovide a broader perspective on cocatalyst properties that influence electron extraction from\nGaN as below:\n(P19) “Beyond the specific Pt/GaN system studied here, in which the metal and semiconductor\nexhibit distinct work functions, interfacial electron-transfer efficiency in GaN-based\nphotocatalytic systems is largely dictated by a combination of cocatalyst properties.\nSpecifically, the semiconductor/cocatalyst band alignment, the chemical nature of interfacial\nbonding, and the ability to passivate surface states collectively dictate the kinetics and\nselectivity of interfacial electron transfer48. This broader perspective helps rationalize why a\nwide range of cocatalysts, including noble metals, transition metals, and metal oxides, can\neffectively facilitate carrier extraction on GaN surfaces.”\nReviewer #2 (Remarks to the Author):\nHere, the systematic regulation mechanism of Pt modification on the ultrafast electron\ndynamics of GaN surface was revealed, especially the discovery of an energy-independent\nelectron injection process of ~50 fs and the revelation of its synergistic enhancement effect\nwith bulk-surface transport. The topic is attractive to the broad readership of Nature\nCommunications. So I recommend this manuscript can be accepted after revisions. And some\nquestions should be addressed as following.\nResponse: We are thankful to the reviewer for appreciating our work and constructive\ncomments. All concerns raised have been carefully addressed, and the suggested revisions have\nbeen incorporated into the updated manuscript.\n1. AFM shows that Pt exists in the form of nano-islands, but no coverage statistics or particle\nsize distribution is provided. It is suggested to supplement the statistical information to\ndetermine whether the distribution of Pt is uniform and whether it forms continuous or discrete\nelectron transmission channels.\nResponse: We thank the reviewer for this valuable suggestion. In response, we performed a\nstatistical analysis of the Pt nano-islands based on AFM image over representative surface areas.\nThe results (Figure R1) show that the Pt nano-islands have an average height size of ~0.73 nm\nwith a surface coverage of ~56%. These data confirm that Pt predominantly remains in the\nform of discrete nano-islands rather than forming a continuous film. Moreover, the\nhomogeneous distribution of nano-islands across the surface provides consistent interfacial\ncontact, ensuring that charge transfer proceeds through localized metal/semiconductor\njunctions rather than continuous metallic channels.\nThese statistical results have been included in Supplementary Fig. 10a in the revised SI, and\nthe corresponding discussion has been added to the revised manuscript as follows:\n(P12) “Statistical analysis of AFM images (Supplementary Fig. 10a) reveals that Pt\npredominantly forms discrete nano-islands with an average height size of ~0.73 nm and a\nsurface coverage of ~56%. The homogeneous distribution across the surface indicates that\ncharge transfer occurs primarily through localized metal/semiconductor junctions rather than\ncontinuous metallic channels.”\nFigure R1. (a) AFM image of Pt nano-islands on GaN substrate. The colours denote different\nheights for Pt nano-islands and GaN terraces (purple). (b) Statistical analysis of height\ndistributions of Pt nano-islands and their Gaussian fits.\n2. Please add TEM/STEM imaging of the Pt/GaN interface.\nResponse: We have examined both TEM and STEM images of the Pt/GaN interface, as shown\nin Figure R2. The TEM results show that the Pt forms discrete nano-islands on the GaN surface,\nexhibiting intimate contact with the underlying GaN substrate. In addition, the STEM\nobservations offer a more refined visualization of the interfacial region, highlighting a sharply\ndefined, microscopically flat, and structurally uniform interface. The TEM/STEM results and\nthe corresponding discussion have been added to the revised manuscript to provide a more\ncomplete characterization of the Pt/GaN interface as follows:\n(P12) “Transmission electron microscopy (TEM, Supplementary Fig. 10b,c) images show that\nthe Pt nanoparticles are uniformly anchored on the GaN substrate with intimate interfacial\ncontact. Moreover, scanning transmission electron microscopy (STEM, Supplementary Fig.\n10d) image reveals a sharply defined, microscopically flat, and structurally uniform Pt/GaN\ninterface.”\nFigure R2. (a,b) Transmission electron microscopy (TEM) images of the Pt/GaN interface. (c)\nHigh-angle annular dark-field scanning transmission electron microscopy (HAADF-STEM)\nimage of Pt/GaN interface.\n3. Fig. 3g shows that the time constants range from 0.5 eV to 2.5 eV, which are indeed very\nclose. However, the data points in the higher energy region (>2.5 eV) seem to be more scattered\nand show a slight upward trend. Please further explain whether this phenomenon is due to\nstatistical errors or if there is indeed a slight energy dependence?\nResponse: Thank you for raising this insightful comment. In Fig. 3g, the time constants in the\nlow- to mid-energy region (0.5–2.5 eV) are indeed very close, reflecting consistent carrier\nrelaxation dynamics. For the higher energy region (>2.5 eV), the observed scatter and slight\nupward trend are primarily attributed to larger statistical uncertainties due to weaker signal\nintensities and lower signal-to-noise ratios in this spectral window. Nevertheless, we note that\nthis reflect a real energy-independent charge transfer, as the thermalization dynamics of hot\nelectrons inherently exhibit significant energy dependence, regardless of whether they\nthermalize in Pt or in GaN. We have added a discussion in the revised manuscript to clarify this\npoint:\n(P13-P14) “Notably, the lifetimes of excited electron typically exhibit strong energy\ndependence in both semiconductors29,30,40 and metals41,42. The absence of such dependence here\nprovides compelling evidence for a uniform ultrafast energy-independent electron transfer\nfrom GaN to Pt, occurring within 41 fs across both DB and CB states.”\n4.In the two-dimensional pseudo-color 2PPE (Fig 4b), the enhancement of low-energy signals\nof Pt/GaN during negative delay is attributed to “bulk phase transport”. Whether this is affected\nby the inter-band transitions of Pt, considering that Pt has strong absorption in the UV-Vis\nregion.\nResponse: Thank you for this thoughtful comment. We agree that Pt exhibits strong interband\nabsorption under the UV excitation used in our study (4.49 eV), which could in principle\ncontribute to photoemission at negative delay. However, both Pt/GaN and bare GaN samples\ndisplay nearly identical spectral shapes at negative delay times (Figure 4d), with the only\ndistinction being an intensity enhancement in Pt/GaN. This strongly suggests that the signal\ncharacteristics are not governed by Pt-specific excitations. Moreover, kinetic analysis of the\nnegative delay signal for Pt/GaN reveals a slower component with a lifetime of 1.96 ± 0.34 ps\n(Figure 4e), which is far longer than the typical tens-of-femtoseconds lifetime of hot carriers\nin Pt that rapidly decay via electron–electron scattering (Phys. Rev. B, 2001, 63, 115420). Taken\ntogether, the consistent spectral features across both samples and the presence of a long-lived\ncomponent provide compelling evidence that the observed signal does not originate from Pt\ninterband transitions. Therefore, any contribution from Pt interband absorption can be\nconsidered negligible in our observed transient signals.\n5. Lines 146-148: The low-energy surface defect states are correlated with Mg-doped defects.\nLine 169: The mid-bandgap defect states are directly attributed to nitrogen vacancies. However,\nthere is a lack of direct characterization (such as EPR).\nResponse: Following the reviewer’s suggestion, we conducted additional EPR measurements\nto directly probe the defect states in GaN. As shown in Figure R3, a pronounced signal at a g\nvalue of 1.9798 is attributed to deep donor states associated with nitrogen vacancies, while a\nweaker signal at a g value of 2.0008 corresponds to shallow acceptor states induced by Mg\ndoping (Phys. Rev. B 2002, 65, 085312; Mater. Sci. Eng. B, 2002, 93, 39–48). These EPR results\nprovide direct experimental confirmation of the defect assignments proposed in our initial\nanalysis. The corresponding data and the relevant discussion have been included in the revised\nmanuscript as below:\n(P8-P9) “In contrast, the transient feature at 0.5 eV is attributed to mid-gap DB states associated\nwith nitrogen vacancies28, as further supported by electron paramagnetic resonance (EPR)\nspectra revealing a pronounced deep donors signal related to nitrogen vacancies\n(Supplementary Fig. 8). These defect-related features in GaN (see Supplementary Fig. 9a for\ndetailed defect distributions) differ significantly from the characteristic gradual population\ntypically observed during defect-state trapping, as observed in Cu O31.”\n6. The photocurrent of Pt/GaN was increased by 6.6 times (Fig. 5c), but no stability data (such\nas the attenuation curve under continuous illumination) was provided. Further stability tests\nshould be conducted. The Faraday efficiency should be supplemented to confirm the\ncorrespondence between H2 production and current.\nResponse: We thank the reviewer for this constructive comment. In response, we conducted\nadditional stability measurements on the Pt/GaN photoelectrode under continuous illumination.\nAs shown in Figure R4, the photocurrent remains stable for over 800 min, demonstrating\nexcellent operational durability of both samples. Furthermore, we evaluated the Faradaic\nefficiency for hydrogen evolution under the same conditions. The Pt/GaN photocathode\nexhibits a Faradaic efficiency exceeding 97% at –0.4 V vs. RHE, confirming that nearly all\nphotogenerated electrons are utilized for the HER. These new results are presented in the\nrevised SI (Figure S22b), and the corresponding discussion has been added to the revised\nmanuscript as follows:\n(P20-P21) “The Pt/GaN photocathode exhibits stable photocurrent for over 800 min under\ncontinuous illumination (Supplementary Fig. 22b), demonstrating excellent operational\ndurability. Moreover, the Faradaic efficiency for H evolution exceeds 97% at –0.4 V vs. RHE,\n2\nconfirming that nearly all photogenerated electrons are consumed in the HER process.”\nFigure R4. Stability test and Faradaic efficiency (solid circles) for GaN and Pt/GaN\nphotocathodes for PEC hydrogen evolution reaction at the applied voltage of -0.4 V vs. RHE.\n7. Is it possible to enhance the mechanistic interpretation through theoretical calculations.\nFor example, predicting the density-of-states distribution at the Pt/GaN interface or\nmodeling the influence of SPV on the band structure.\nResponse: We thank the reviewer for the suggestion. To provide further mechanistic support\nfor charge transfer, we carried out simplified device-level simulations of the band bending and\nsurface photovoltage (SPV) at the GaN surface under illumination. Our approach is based on\nsolving the one-dimensional Poisson–drift–diffusion equations, which describe electrostatics\nand carrier transport in n-type GaN.\nSpecifically, the electrostatic potential (𝜑(𝑥)) was obtained from Poisson’s equation:\n𝑑2𝜑(𝑥) 𝜌(𝑥)\n= −\n𝑑𝑥2 𝜀\nwhere 𝜌(𝑥) = 𝑞(𝑝(𝑥)−𝑛(𝑥)+𝑁+ −𝑁−) is the local space charge density, 𝑞 is the\n𝐷 𝐴\nelementary charge, and 𝜀 = 9 is the dielectric constant of GaN. 𝑁+ and 𝑁− denote the densities\n𝐷 𝐴\nof ionized donors and ionized acceptors, respectively. The electron and hole current densities\nare described by the drift–diffusion equations:\n𝑑𝑛(𝑥)\n𝐽 (𝑥) = 𝑞𝜇 𝑛(𝑥)𝐸(𝑥)+𝑞𝐷 ,\n𝑛 𝑛 𝑛 𝑑𝑥\n𝑑𝑝(𝑥)\n𝐽 (𝑥) = 𝑞𝜇 𝑝(𝑥)𝐸(𝑥)−𝑞𝐷 ,\n𝑝 𝑝 𝑝 𝑑𝑥\nwhere 𝑛(𝑥) and 𝑝(𝑥) are the electron and hole concentrations, 𝜇 and 𝜇 are carrier mobilities,\n𝑛 𝑝\n𝐷 and 𝐷 are charge diffusion coefficients, and 𝐸(𝑥) = −𝑑𝜑(𝑥)/𝑑𝑥 is the electric field\n𝑛 𝑝\ndistribution. In this coupled framework, Poisson’s equation links the local potential to carrier\ndensities, while the drift–diffusion and continuity equations determine how photogenerated\ncarriers redistribute and screen the built-in field. Thus, these equations allow us to calculate\nboth the equilibrium band bending (dark state) and the modified potential profile under\nillumination. The simulation results are presented in Figure R5. In the dark, the GaN surface\nshows an upward band bending of ~0.35 eV. Upon UV illumination, this band bending at the\nGaN surface is reduced by ~0.1 eV, in good agreement with our tr-2PPE observation of band\nflattening. Moreover, the calculated SPV increases with light intensity and gradually saturates\nat higher fluence, reflecting the effective screening of the built-in field by photogenerated\ncarriers. We have added the corresponding figure in the SI (Supplementary Fig. 5d,e) and\nrelevant discussion in the revised manuscript as below:\n(P10) “This interpretation is further supported by simplified simulations (Supplementary Fig.\n5d,e), which reproduce the experimentally observed band flattening and show that bandgap\nillumination reduces the upward band bending at the GaN surface by approximately 0.1 eV.”\nFigure R5. (a) Band bending profiles at the GaN surface in the dark and under illumination,\nillustrating the band-flattening effect induced by photoexcitation. (b) Light-intensity-\ndependent SPV curve for the GaN surface under bandgap excitation, showing that the SPV\nincreases with illumination intensity and gradually saturates.\nReviewer #3 (Remarks to the Author):\nUsing the state-resolved tr-2PPE spectroscopy, the authors uncovers the ultrafast carrier\nrelaxation dynamics in GaN-based photocatalysts and demonstrates how interfacial\nengineering via Pt modification fundamentally redefines the energetic landscape and transport\nbehavior at the metal/semiconductor junction. However, the manuscript needs further revisions\nto clarify the following points:\nResponse: We thank the reviewer for the positive assessment of our work. We have carefully\nrevised the manuscript to clarify the points raised and believe that the changes improve both\nthe clarity and impact of the study.\n(1) What causes deep level defects at the Fermi level? Please provide a detailed explanation.\nResponse: We appreciate the reviewer for raising a point similar to that of Reviewer #2\nregarding the origin of deep-level defect states near the Fermi level. In n-type GaN, deep-level\ndefect states near the Fermi level predominantly arise from intrinsic point defects and doping\ndefects. In particular, nitrogen vacancies (V ) are well known to act as deep donors, introducing\nN\nelectronic states near the conduction band minimum that are often pinned close to the Fermi\nlevel in moderately doped samples (Appl. Phys. Lett. 1996, 69, 2525–2527; Appl. Phys. Lett.\n2012, 100, 142110; Materials 2024, 17, 1160). Additionally, Mg dopants can generate acceptor-\nlike defect states that, when partially compensated, contribute to defect levels within the\nbandgap (Phys. Rev. Lett. 2015, 114, 016405). The coexistence of these donor- and acceptor-\nrelated defects gives rise to localized states near the Fermi energy. Importantly, we have\nperformed EPR measurements that show a pronounced signal at g = 1.9798, consistent with\nnitrogen-vacancy–related deep donors, and a weaker signal at g = 2.0008 consistent with Mg-\ninduced acceptors (Figure R3). The observed spectroscopic signatures indicate that the mid-\ngap features detected in tr-2PPE can be attributed to nitrogen-vacancy-related states. A detailed\nexplanation has been incorporated into the revised manuscript as follows:\n(P8-P9) “In contrast, the transient feature at 0.5 eV is attributed to mid-gap DB states associated\nwith nitrogen vacancies28, as further supported by electron paramagnetic resonance (EPR)\nspectra revealing a pronounced deep donors signal related to nitrogen vacancies\n(Supplementary Fig. 8). These defect-related features in GaN (see Supplementary Fig. 9a for\ndetailed defect distributions) differ significantly from the characteristic gradual population\ntypically observed during defect-state trapping, as observed in Cu O31.”\n2\n(2) Does the conclusion of 'energy independent charge extraction' hold true in other materials\nas well, or is it only observed in GaN?\nResponse: We thank the reviewer for this important comment. The observation of energy-\nindependent charge extraction has been experimentally demonstrated here for the Pt/GaN\nsystem. While the current results are specific to GaN, the underlying mechanism is likely\napplicable to other metal/semiconductor heterostructures with similar interface properties.\nNevertheless, the universality of this phenomenon remains to be verified experimentally in\nother materials, as factors such as energy band structure, interfacial chemical bonding, and\ninterface states may collectively influence the energy dependence of charge extraction. This\nwork establishes a broadly applicable framework for elucidating ultrafast, energy-resolved\ninterfacial charge dynamics in metal/semiconductor heterostructures, serving as a guiding\nparadigm for studies in alternative material platforms.\n(3) In the introduction section, the authors described that “Despite their impressive\nperformance, the details of how such surface modifications alter the ultrafast energy relaxation\npathways of photoexcited carriers are still unclear.” The unclear question lies in which aspects,\nas research in this field is already very common. The author did not mention the significant\nsignificance and necessity of the research.\nResponse: We thank the reviewer for highlighting this point. While surface modification of\nsemiconductors has been extensively explored, the ultrafast energy-resolved dynamics of\nphotoexcited carriers at modified interfaces remain poorly understood. In particular, it is\nunclear how metal/semiconductor junctions alter the partitioning between nonthermal and\nthermalized electrons during charge transport, the timescales of energy relaxation, and state-\nspecific charge separation mechanism. Our study addresses this gap by employing femtosecond\ntime-resolved two-photon photoemission (tr-2PPE) spectroscopy, providing simultaneous\ntemporal and energy-resolved insights into carrier dynamics. These measurements offer a direct\nmechanistic understanding of how interface engineering modulates nonequilibrium electron\nbehavior, thereby guiding rational design of cocatalysts and interfaces to maximize charge\nseparation and photocatalytic efficiency. Thus, our study addresses an important gap in linking\nsurface modification to ultrafast carrier behavior with energy and time resolution, which has\nnot been comprehensively explored in previous reports.\nWe have revised the Introduction to better clarify the central research question and to highlight\nboth the significance and necessity of this study as below:\n(P3) “…, most studies have focused on bulk carrier behaviors or averaged interfacial processes,\nwhereas the femtosecond energy relaxation pathways at metal/semiconductor interfaces remain\npoorly understood. In particular, it is not well established how surface modifications alter the\ninitial energy distribution, defect trapping, and interfacial injection of hot carriers immediately\nafter photoexcitation. This knowledge gap is critical because only carriers that retain sufficient\nexcess energy on ultrafast timescales can efficiently participate in catalytic reactions.”\n(P4) “These hybrid catalysts benefit from engineered metal/semiconductor interfaces that\noptimize interactions between catalytic sites and reaction intermediates, reduce kinetic barriers,\nand improve charge separation. Despite these advances, the mechanistic details of how such\nmetal/semiconductor interfaces reshape the ultrafast carrier energy landscape remain elusive.\nSpecifically, the formation of a metal/semiconductor junction introduces new interfacial\nstates14,22 that modulate the built-in electric field and band alignment23,24, thereby influencing\nthe carrier energy landscape and transport behavior. Yet these effects have rarely been studied\nwith sufficient energy and time resolution sufficient to capture energy-resolved ultrafast charge\ndynamics.”\n(P5) “Our results provide direct mechanistic insight into how interface engineering preserves\nhot carrier energy and enhances bulk-to-surface transport, offering a framework for rational\ndesign of cocatalysts and semiconductor interfaces to improve photocatalytic efficiency.”"}, {"round": 2, "reviewer_comments": {"reviewer_1": "The authors have provided clear responses to my comments. The revised manuscript strengthens the logical flow of the\ndiscussion and acknowledges the limitations of UHV-based measurements when compared with realistic PEC\nenvironments. The added clarifications on possible surface oxidation and its influence on band bending and charge-transfer\ndynamics provide valuable context.\nWhile additional experiments such as probing carrier dynamics on intentionally oxidized surfaces or comparing different\ncocatalysts with varied work function would deepen the mechanistic understanding, I believe that the current results already\noffer important scientific insights. The manuscript convincingly demonstrates key aspects of interfacial charge transport and\nthe role of Pt in modulating carrier dynamics at GaN surfaces. Therefore, I recommend the manuscript for acceptance in its\ncurrent form.", "reviewer_2": "I agree that it can be accepted for publication.", "reviewer_3": "The author has already answered the questions I raised."}, "author_response": ""}]

Decision letter