Surface photovoltage spectroscopy (SPS) measures illumination-induced contact potential difference (CPD) change as a function of photon energy. Unlike optical absorption, which detects photon attenuation, SPS probes charge separation within the surface depletion region. The signal is weighted by carrier generation, diffusion, drift, trapping kinetics, and band bending rather than optical cross section alone, enabling detection of defect-mediated sub-bandgap transitions and photovoltaic potential invisible to absorption spectra. Quantitative interpretation requires declared measurement conventions, explicit band-bending models, independent material verification, and awareness that surface chemistry, moisture, temperature, and illumination history continuously modulate the observed signal.

Surface photovoltage is defined as contact potential difference shift from dark to illuminated under a declared sign convention. The fundamental signal is $$\mathrm{SPV}(h\nu)=\mathrm{CPD}_{\mathrm{light}}(h\nu)-\mathrm{CPD}_{\mathrm{dark}},$$ where CPD is measured via Kelvin probe under the convention $$\mathrm{CPD}=\frac{\Phi_{\mathrm{probe}}-\Phi_{\mathrm{sample}}}{e}$$ or its opposite. Absolute values are reference-dependent; SPS amplitude reflects net charge separation rather than intrinsic properties. Dark CPD +0.35 V and illuminated +0.47 V yields 120 mV SPV under the adopted convention—condition-specific, reflecting photogeneration, carrier separation, and recombination equilibrium. Sign indicates whether holes or electrons accumulate at the surface under the declared band-bending and illumination geometry.

Photon-energy calibration and monochromator bandwidth control sub-bandgap and bandgap-onset interpretation. Wavelength-energy conversion $$E_\gamma(\mathrm{eV})=\frac{1239.84}{\lambda(\mathrm{nm})}$$ is exact: 620 nm = 2.00 eV. An energy sweep from 1.50–3.00 eV in 0.005 eV steps yields $$N_{\mathrm{points}}=\frac{3.00-1.50}{0.005}+1=301 \text{ points}.$$ At 2 seconds per point, raw dwell is 602 seconds before monochromator settling and dark references. Higher-order light and stray radiation corrupt sub-bandgap assignments; order-sorting filters are mandatory. Constant photon flux (not constant power) prevents short-wavelength undersampling, and detector drift must be tracked via repeated references.

Above-gap and sub-gap response require distinct interpretation frameworks because optical absorption, defect density of states, surface Fermi-level, and recombination shape the observed spectrum. Above bandgap (E > E_bg), onset correlates with band-to-band transitions, modulated by temperature (Urbach tails) and band structure. Sub-gap features reflect defect-mediated transitions; surface defects dominate over bulk (Kelvin-probe spatial average ~100 nm). A sub-gap SPS feature does not identify defect species, concentration, or depth without independent data. Correlation with XPS/UPS (Fermi-level position), photoluminescence (recombination pathways), and DLTS (deep-level profiling) is essential for credible defect assignment.

Carrier-diffusion length, depletion width, and optical absorption depth establish spatial signal origin and must be specified for quantitative modeling. An electron-hole pair at depth z contributes to SPS only if it reaches the space-charge region before recombining. Diffusion length L_diff (typically 100 nm–10 μm) sets the spatial cutoff; deeper carriers are lost to bulk recombination. Depletion width W_depl ranges ~10 nm (degenerately doped) to ~1 μm (lightly doped). Optical absorption coefficient α(hν) at 620 nm in direct-gap oxides is ~10⁴–10⁵ cm⁻¹, with intensity decaying to 1/e within 0.1–1 μm. Observed SPS is depth-weighted carrier collection efficiency across the light-absorbing and drift-collecting region.

Modulation frequency, lock-in time constant, and scan direction reveal kinetics—trap-mediated recombination, persistent photoconductivity, light-soaking—inaccessible to static acquisition. DC SPS measures equilibrium photovoltage after >30 min dark/light equilibration. Modulated SPS applies intensity modulation (typically 50–250 kHz) and measures CPD amplitude/phase via lock-in. Fast response (μs–ms) indicates mobile carriers; slow response (s–min) indicates trapping. Scan-direction reversal exposes hysteresis. Light-soaking shifts SPS amplitude via trap occupancy and adsorbate modification. Dark-recovery tests reversibility versus permanent deep trapping.

Semiconductors, oxides, perovskites, organics, and 2D materials exhibit distinctive SPS signatures shaped by band structure, defects, and surface chemistry. Silicon and GaAs map equilibrium band bending; correlate with C–V and open-circuit voltage. Metal oxides (TiO₂, SrTiO₃, WO₃, BiVO₄) show strong sub-bandgap features from oxygen vacancies and reduced-metal sites; amplitude sensitive to hydroxylation and adsorbates. Halide perovskites (CH₃NH₃PbI₃, CsPbI₃) exhibit large SPV but drift over minutes due to ionic migration. Organics show weak SPS (low diffusion length, high recombination) but reveal HOMO–LUMO states and interface dipoles. Graphene and dichalcogenides generate SPV via photo-induced Fermi shifts and exciton dissociation. No universal defect-concentration algorithm exists; material-specific physics and independent calibration are essential.

Quantitative defect interpretation requires simultaneous band-bending model (C–V/Mott–Schottky), work-function verification (UPS), majority-carrier data (Hall/4-point probe), and minority-carrier data (photoluminescence/EQE). Sub-gap SPS cannot convert to defect concentrations without surface Fermi-level position (UPS valence, core-level XPS), band bending under illumination (C–V), and transition cross sections (photon-flux dependence, photoluminescence). Without these anchors, SPS remains a phenomenological descriptor; no unique defect assignment exists. Claims like "50 mV sub-gap feature = 10¹² cm⁻³ oxygen vacancies" apply only within specific material, surface preparation, and defect model. General conversion factors fail because SPS amplitude depends nonlinearly on photon flux, surface occupancy, and band bending—conditions varying between labs and samples.

Environment—humidity, temperature, oxygen/moisture adsorbates—shifts CPD by 50–200 mV and must be controlled and documented. Vacuum-cleaved surfaces differ from air-exposed by 50–200 mV (oxygen chemisorption, hydroxylation, water). Humidity (20–80% RH) shifts CPD by 100+ mV in sensitive materials. Temperature coefficient is ~1–3 mV/K. Noncontact measurement is not nonperturbing: probe fields and illumination modify surface occupancy continuously. Measurements must specify chamber pressure, humidity (logged), temperature stability (±1 K), spot geometry, and time since preparation. Identical samples at 40% RH/25 °C (air) versus <10⁻⁶ Torr (vacuum) show fundamentally different CPD and SPS due to adsorbate layers and Fermi-level pinning.

Define measurement goal (band bending, defect detection, or photovoltaic potential) → Select Kelvin-probe system and declare sign convention in advance → Prepare sample: document preparation method, surface composition, native oxide or adsorbate layer (AFM, XPS, ellipsometry) → Establish environmental control: seal chamber, log humidity/temperature continuously, set temperature stability ±1 K → Calibrate Kelvin-probe work function using certified reference standard before and after sample series → Acquire C–V or Mott–Schottky data on same sample region to constrain band bending and flatband voltage → Prepare for dark equilibration: enclose sample in opaque chamber for >30 min → Acquire dark-state Kelvin-probe map (20–30 points) with repeated reference measurements → Illuminate sample with filtered/monochromatic light from 1.50 eV to 3.00 eV in 0.005 eV steps (301 points) → At each energy: allow >2 min equilibration, then measure CPD via lock-in detection (2 s dwell); record photon flux and monochromator bandwidth → Reverse scan direction to assess hysteresis → Acquire steady-state SPV by computing (illuminated − dark) CPD at each energy → Correlate SPS spectrum with XPS/UPS (Fermi-level position, band offset), photoluminescence (recombination channels), DLTS or capacitive spectroscopy (deep-level profiling) → Compare SPS onset energy with UV-Vis absorption edge and with band-bending predictions from C–V → If semiconductor or photovoltaic device: correlate with open-circuit voltage, external quantum efficiency, and Fermi-level splitting under illumination → Document all environmental parameters, probe history, and measurement settings → Report SPS spectrum with declared sign convention, absolute values only under stated reference calibration, explicit caveats on defect attribution, and reproducibility uncertainty

Read surface photovoltage spectroscopy through a generation-separation-kinetics lens: SPS measures the illumination-induced shift in contact potential difference as a function of photon energy and quantifies charge separation driven by photogeneration and spatial drift in the surface depletion region. Unlike optical absorption spectra, which report photon attenuation, SPS is fundamentally weighted by carrier-generation efficiency, diffusion and drift lengths, trap-mediated recombination kinetics, and band-bending dynamics—enabling detection of optically dark defect-mediated transitions and photovoltaic potential. An illustrative example at 620 nm (E = 1239.84/620 = 2.00 eV) shows dark CPD +0.35 V and illuminated CPD +0.47 V, yielding 120 mV SPV under a declared convention; this magnitude is condition-specific and reflects partial band flattening rather than the entire built-in potential. Measurement from 1.50 to 3.00 eV in 0.005 eV steps requires 301 points at 2 seconds per point, totaling 602 seconds ideal dwell (~10 minutes) before modulation settling and dark references. Sub-bandgap SPS features reveal defect-mediated transitions but do not uniquely identify defect species, concentration, spatial depth, or transition energy without complementary XPS/UPS (Fermi-level position and valence-band offset), C–V analysis (band bending and carrier density), photoluminescence (recombination mechanisms), and DLTS (deep-level profiling). Environmental adsorbates, humidity, and temperature each shift measured CPD by tens to hundreds of millivolts independently of intrinsic material properties; quantitative interpretation requires explicit control, continuous logging, and acknowledged uncertainty. Noncontact measurement does not guarantee non-perturbing conditions: the probe field and illumination modify surface occupancy and adsorbate equilibrium continuously. Credible SPS interpretation integrates measurement of surface Fermi-level position and band-bending geometry with multi-technique correlation, declared sign convention throughout, and honest uncertainty in defect attribution pending independent verification via spectroscopy or device characterization.