Geoscientist Artificial Intelligence
Geoscientist Artificial Intelligence
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  • Processing & Imaging
    • Anisotropy Analysis
    • Deconvolution
    • Inverse Q Filtering
    • Migration
    • Multiple Attenuation
    • Noise Attenuation
    • Ray Tracing
    • Stacking
    • Static Correction
    • Velocity & NMO Analysis
    • Waveform Modeling
    • Wave Equation Datuming
  • Q-Interpretation
    • AVO Analysis
    • Data Conditioning
    • Facies Analysis
    • INVERSION
    • Rock Physics Modeling
    • Seismic Attributes
    • Spectral Blending
    • Time to Depth Convrsion
  • More
    • Home
    • Processing & Imaging
      • Anisotropy Analysis
      • Deconvolution
      • Inverse Q Filtering
      • Migration
      • Multiple Attenuation
      • Noise Attenuation
      • Ray Tracing
      • Stacking
      • Static Correction
      • Velocity & NMO Analysis
      • Waveform Modeling
      • Wave Equation Datuming
    • Q-Interpretation
      • AVO Analysis
      • Data Conditioning
      • Facies Analysis
      • INVERSION
      • Rock Physics Modeling
      • Seismic Attributes
      • Spectral Blending
      • Time to Depth Convrsion
  • Home
  • Processing & Imaging
    • Anisotropy Analysis
    • Deconvolution
    • Inverse Q Filtering
    • Migration
    • Multiple Attenuation
    • Noise Attenuation
    • Ray Tracing
    • Stacking
    • Static Correction
    • Velocity & NMO Analysis
    • Waveform Modeling
    • Wave Equation Datuming
  • Q-Interpretation
    • AVO Analysis
    • Data Conditioning
    • Facies Analysis
    • INVERSION
    • Rock Physics Modeling
    • Seismic Attributes
    • Spectral Blending
    • Time to Depth Convrsion

seismic data conditioning

Seismic data conditioning on post-stack data is a crucial step in preparing migrated or stacked seismic sections for interpretation, attribute analysis, and inversion. The goal is to enhance the signal, improve continuity, and reduce noise or artifacts that may obscure geological information. Here’s a structured summary of the main methods of post-stack seismic data conditioning grouped by purpose:

🧭 1. Amplitude and Phase Conditioning

Purpose: Correct amplitude and phase distortions to make reflections true to the subsurface.

  • Spectral balancing / Whitening:
    Balances frequency content to enhance resolution. Often done by flattening the amplitude spectrum across frequencies.
  • Phase correction / zero-phasing:
    Converts data to zero phase (wavelet centered on reflection), improving reflector positioning and correlation with well data.
  • True-amplitude recovery (gain correction):
    Applies time-variant scaling (e.g., AGC or t² gain) or inverse spherical divergence correction to compensate for amplitude decay with time.

Amplitude and Phase Conditioning

Result of applying AI seismic spectral balancing.

Seismic spectral balancing is a broadband enhancement technique that flattens the amplitude spectrum of seismic traces to compensate for source band-limitation, earth filtering, and frequency-dependent attenuation (Q-loss). The method works by dividing the data into overlapping time windows, computing each window’s smoothed amplitude spectrum, and constructing a frequency-dependent gain operator that boosts weaker high frequencies and moderates strong low frequencies. Applying this operator in the frequency domain and reconstructing the trace produces a more uniform (“white”) spectrum that improves vertical resolution and reflector continuity. 

Time-variant spectral balancing applies progressively stronger high-frequency boosting with depth to counter increasing attenuation. While effective and stable compared to physical Q-compensation, spectral balancing can amplify noise and requires parameter control (window length, smoothing, whitening power, stabilizer) to avoid over-whitening or amplitude distortion.

Result of applying AI seismic zero phasing

Seismic zero-phasing is a wavelet-shaping process that adjusts each seismic trace so the embedded source wavelet becomes zero-phase, meaning its energy is centered at time zero and reflection events align with their true subsurface positions. Because real seismic data typically contains a mixed-phase or minimum-phase wavelet due to source signature, instrument response, and earth absorption, zero-phasing estimates the wavelet's phase spectrum often using statistical methods such as autocorrelation, spectral ratio, or spiking deconvolution and then applies a phase-correction operator in the frequency domain to remove the estimated phase and force the wavelet to zero phase. The operation is typically time-variant and windowed to account for phase changes with depth. 

Zero-phasing improves reflector interpretability, sharpens events, and aligns peaks and troughs with impedance contrasts, but requires careful wavelet estimation; inaccurate phase correction can distort amplitudes, misalign events, or introduce artifacts, especially in low-SNR or strongly attenuated intervals.

Result of applying ai seismic Amplitude Gain

Amplitude gain in seismic processing is a family of techniques that compensate for time-dependent energy decay caused by geometric spreading, intrinsic attenuation, absorption, and transmission losses as waves travel deeper into the subsurface. Since deeper reflections naturally have lower amplitudes, gain functions such as AGC (Automatic Gain Control), true-amplitude spherical divergence correction, exponential or power-law time-variant gains, and structure-consistent scaling are applied to equalize amplitudes across the trace. These methods typically compute a windowed or global envelope, derive a gain factor that boosts weaker parts of the signal, and apply it in the time domain to restore relative visibility of deep events. Proper amplitude gain improves reflector continuity, enhances interpretability, and stabilizes subsequent processes like filtering and migration. However, excessive or poorly designed gain can distort true amplitude relationships, mask AVO effects, exaggerate noise, or create artificial continuity; therefore gain type, window length, and stabilization parameters must be chosen carefully to preserve geologic amplitude fidelity.

🧼 2. Noise Attenuation

Purpose: Suppress random and coherent noise without damaging signal.

  • FX deconvolution / FX smoothing: Operates in frequency–space domain to enhance lateral continuity and reduce random noise.
  • Structure-oriented filtering (SOF): Preserves geological features by filtering along dip directions (e.g., dip-steering filters).
  • Median filtering: Useful for spike or burst noise removal while keeping edge sharpness.
  • Kx-Kz or FK filtering: Removes linear noise or migration artifacts in frequency–wavenumber domain.
  • Dip filter: Suppresses events outside desired dip range, e.g., migration smiles or multiples.

noise attenuation in data conditioning

Result of applying AI seismic FX Deconvolution

FX deconvolution is a frequency–space domain technique for suppressing random noise and enhancing coherent seismic events by exploiting the fact that true reflections vary smoothly across traces, while random noise is uncorrelated trace-to-trace. The method transforms each time window of the seismic section into the FX domain via FFT along the time axis; at each frequency slice, the complex amplitudes across traces are modeled as a predictable, low-order autoregressive (AR) process. The AR coefficients are estimated using least-squares or stabilized prediction-error filters, and the predicted coherent signal is reconstructed while the unpredictable energy random noise is attenuated. After inverse FFT to the time domain, the output section exhibits improved continuity and reduced random noise. FX deconvolution works best when events are linear and coherent, but requires proper AR model order, window size, and stabilizers; if poorly tuned, it can leave residual noise, distort dipping events, or introduce frequency-dependent artifacts, especially in low-SNR or aliased data.

Result of applying AI seismic dip steering filter.

A dip-steering filter is a structure-oriented smoothing method that enhances seismic continuity while preserving true reflector geometry by guiding the filtering process along locally estimated dips instead of vertically or laterally. First, a dip field is computed using gradient, semblance, or plane-wave destruction methods to determine the local slope of seismic events at each sample. Using this dip field, the filter constructs a steerable window that follows the reflector orientation, and then applies weighted averaging or tensor-based smoothing along the dip direction while minimizing mixing across conflicting dips. This suppresses random noise and small-scale incoherent features while maintaining faults, terminations, and stratigraphic details. 

Dip-steered filtering is highly effective for horizon interpretation, attribute calculation, and preconditioning before inversion, but requires accurate dip estimation; poor or noisy dip fields can create smearing, leakage across faults, or artificial structures.

Result of applying ai seismic dip-guided median filter.

A dip-guided median filter is a structure-oriented noise-reduction technique that combines the robustness of median filtering with the directional preservation provided by dip estimation. First, a local dip field is computed using methods such as plane-wave destruction or gradient-based slope analysis to determine the orientation of seismic reflectors at each sample. Using this dip field, the algorithm extracts a window of samples aligned along the reflector dip rather than in a vertical or fixed rectangular neighborhood. The median of the samples within this steerable, dip-aligned window is then assigned to the central sample, which effectively suppresses spike noise, burst noise, and small incoherent events while maintaining reflector continuity and protecting edges, terminations, and faults. Because the median operator is non-linear and resistant to outliers, dip-guided median filtering performs better than amplitude-based smoothing when random spikes or high-amplitude noise are present. However, its success depends on accurate dip estimation; poor dip fields or strong conflicting dips may cause reflector distortion or over-smoothing.

🧩 3. Resolution Enhancement

Purpose: Improve vertical and lateral resolution of reflectors.

  • Spectral enhancement / Deconvolution:Expands the bandwidth by inverse filtering or spectral shaping.
  • Thin-bed tuning correction:Adjusts for constructive/destructive interference in thin layers.
  • High-frequency boosting with Q-compensation:Compensates attenuation effects caused by anelastic losses.

🌈 4. Amplitude Preservation and Balancing

Purpose: Prepare data for amplitude-sensitive studies like AVO or inversion.

  • Surface-consistent amplitude correction:Balances amplitudes between traces (accounting for source/receiver effects).
  • Relative amplitude balancing (RAB):Normalizes trace or window amplitudes to minimize lateral variation unrelated to geology.
  • Envelope balancing:Ensures consistent envelope levels for attribute extraction.

🧠 5. Structural and Continuity Enhancement

Purpose: Improve structural coherence and reflector continuity.

  • Structure-oriented smoothing (SOS):Applies smoothing guided by local dip to enhance horizons while preserving faults.
  • Tensor-based or dip-steering filtering:Adaptive filtering based on orientation tensors or local slope analysis.
  • Cadzow or rank-reduction filtering:Enhances coherency by reconstructing low-rank signal subspace.

🧮 6. Attribute Preparation / Interpretation Conditioning

Purpose: Optimize the data for advanced interpretation.

  • Horizon flattening and residual noise removal:Used for spectral decomposition or facies analysis.
  • Spectral decomposition preprocessing:Ensures consistent bandwidth and phase before frequency-based interpretation.
  • Detrending or residual multiple suppression:Removes residual long-period noise or migration artifacts.

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