We use cookies to ensure our website works properly and to personalise your experience. Cookies policy
Department of Statistics, Pondicherry University, Puducherry, India 605014
This research aims to make a substantive contribution to this objective by conducting a comprehensive analysis of seismic activity throughout India, utilizing robust datasets sourced from the official repository of the National Center for Seismology, Government of India. Central to this investigation is the application of advanced stochastic process theory, particularly the deployment of Poisson models to characterize earthquake occurrences. Acknowledging that aftershock sequences inherently contravene the independence postulate of the classical Poisson framework, this study employs refined clustering algorithms. Specifically, the adoption of the Omori-Utsu law facilitates the rigorous segregation of mainshock events, whose inter-occurrence intervals are subsequently demonstrated to adhere closely to a Poissonian temporal distribution. An earthquake constitutes a sudden and often devastating perturbation of the Earth's surface, precipitated by the abrupt release of accumulated seismic energy within the planet's crust. The imperative to systematically study earthquakes extends far beyond academic curiosity, underpinning the disciplines of seismic hazard analysis and risk mitigation, which are foundational for safeguarding both human lives and critical infrastructure. In a geodynamically active nation like India, the development of sophisticated predictive models is of paramount importance due to the heightened vulnerability of densely populated regions.
Earthquake sequences exhibit three primary patterns: (1) foreshock-mainshock-aftershock sequences, (2) mainshock-aftershock sequences, and (3) earthquake swarms characterized by the absence of a dominant event [2]. The statistical characterization of these se- quences poses unique challenges for seismic hazard analysis, particularly concerning their temporal distribution.
Foreshocks and aftershocks are generally lower-magnitude events that cluster tempo- rally around a mainshock. This clustering fundamentally violates the Poisson assumption of independent event occurrences. Michael (1997) demonstrated this phenomenon and suggested the use of autoregressive methods to model aftershock sequences [3]. The non- Poissonian nature of earthquake occurrence has prompted the exploration of alternative modeling approaches, such as Markov and semi-Markov processes, as detailed by Anagnos et al (1988) [1].
The temporal scope of aftershock activity remains an area of ongoing research. Utsu (1961) laid the groundwork for understanding magnitude-dependent aftershock duration, and subsequent studies have further refined these temporal parameters [5]. In this study, we conduct a comprehensive analysis of earthquake sequences across all Indian states, employing various methodologies, including truncation, simple clustering, and Omori- Utsu law-based clustering techniques. This multifaceted approach aims to enhance our understanding of seismic activity patterns and improve seismic hazard assessments.
The data was collected from the official website of the National Center for Seismology, Ministry of Earth Sciences, Government of India. The dataset contains a complete history of earthquakes that originated in India or neighboring countries during the period from 16-04-2013 to 31-05-2025.
The dataset contains earthquake records with the following key columns:
Initially, the dataset featured a column named Location, which contained the complete address of the earthquake origin. For the purpose of this study, this column was split into three separate columns:
This restructuring facilitates clearer insights by categorizing the earthquake data ge- ographically.
As this study exclusively examines earthquakes that originated in India, all instances of earthquakes from neighboring countries have been removed from the dataset. This filtering ensures that the analysis remains pertinent and prevents the introduction of irrelevant data.
To streamline data handling and enable focused analysis, the dataset has been divided into several CSV files. Each file contains the historical records of earthquakes for a single state. This approach improves the organization of the data and allows for state-specific analyses.
All subsequent data processing tasks are conducted in the R programming environment, renowned for its statistical capabilities.
The Magnitude column presented an initial challenge, as it was formatted as alphanu- meric due to the presence of units. This column has been converted into a numeric format to ensure accurate quantitative analysis.
Additionally, a new column titled Interarrival Time has been introduced. This column provides the time interval between successive earthquake occurrences. It is important to note that the calculation of interarrival times is contingent upon the clustering algorithm utilized, which will be discussed further in subsequent sections of this report.
The process begins with data loading and cleaning. Earthquake data from multiple CSV files are read, ensuring that there is a valid ’time’ column, which is essential for time-based analysis. Timestamps are converted into a standardized datetime format to accommodate various date-time input patterns. Rows with missing or malformed time entries are removed to maintain data integrity. Additionally, magnitude values are sanitized to retain only their numeric components, eliminating any appended text or symbols.
Once the data is cleaned and standardized, the next step involves calculating inter- arrival times—the time intervals between successive earthquake events (specifically, daily maximums, which will be discussed separately). These inter-arrival times are expressed in days and serve as the primary metric for examining the temporal structure of the event sequence.
The Poisson process rate parameter λ is then estimated. It is calculated as the ratio of the total number of earthquake events to the total duration (in days) between the first and last events in the data set. The λ value provides a measure of the average number of events per unit time, which is a key parameter for modeling the events under the Poisson framework.
To validate the assumption of a Poisson process, the study employs the Kolmogorov–Smirnov (KS) test. This test compares the empirical distribution of the calculated inter-arrival times with the theoretical exponential distribution, which is characteristic of inter-arrival times in a Poisson process. A high p-value (typically above 0.05) from the KS test indi- cates a good fit, supporting the hypothesis that the events occur according to a Poisson process. Conversely, a low p-value suggests a deviation from this assumption.
Finally, for each processed dataset, the script records key outcomes, such as the esti- mated Poisson rate (λ), the KS test p-value, and a summary interpretation of the KS test result. These findings are compiled into a master results table and saved to an output CSV file for further analysis and documentation. This methodology ensures a consistent and statistically rigorous assessment of the temporal behavior of earthquake occurrences across multiple datasets.
We tried three different approaches to manage the aftershocks which are described in the coming sections
The basic model utilizes a straightforward method for detecting mainshocks. It identifies the most significant earthquake (based on magnitude) that occurs on each calendar day. This is achieved by grouping the dataset by date and selecting the highest-magnitude event from each group. The underlying assumption is that only one important seismic event can occur per day, while any additional events are likely less significant or considered aftershocks. Although this method is computationally efficient and easy to implement, it may oversimplify actual seismic behavior. It does not account for the possibility of two or more independent mainshocks occurring on the same day, particularly in regions with high seismic activity.
While many researchers attempt to predict the time intervals during which aftershocks may occur, there is no definitive rule for determining these periods. However, it is un- derstood that the aftershock period is directly proportional to the magnitude of the mainshock. With this in mind, a clustering rule is defined to manage aftershocks.
The second version adopts a more sophisticated and physically realistic method for identifying mainshocks. It clusters earthquakes based on dynamically assigned time win- dows, which are determined by the magnitude of each potential mainshock. This ap- proach is based on the premise that larger earthquakes tend to produce longer aftershock sequences. For instance, a magnitude 6 earthquake might define a clustering window of ±21 days, whereas a smaller earthquake might only cluster nearby events within ±5 days.
Within each window, the highest-magnitude event is designated as the mainshock, and all surrounding events are considered part of its aftershock sequence. These aftershock windows can be found in [4], and for this study are defined as follows:
This method helps to avoid double-counting related seismic activity and filters out af- tershocks more effectively than the calendar-based approach. However, it comes with increased computational complexity due to the iterative looping and reassignment of events. Despite being more resource-intensive, this version provides a better representa- tion of independent seismic events and aligns more closely with physical seismic models.
Earthquakes with a magnitude less than 5 are generally not felt significantly, and the damage they cause is minimal. Keeping this in mind, the third approach models only destructive earthquakes, which helps manage aftershocks automatically.
In this third version, we introduce a magnitude-based filtering step before identifying mainshocks. Only earthquakes with a magnitude greater than 5 are retained, effectively removing lower-magnitude events and potential noise from the analysis. This step ensures that the dataset focuses solely on moderate to large seismic events, which are more likely to be independent mainshocks rather than aftershocks. After filtering, the code groups the remaining events by the floored date5 and selects the largest magnitude event within each 24-hour period. Although this method resembles the logic of the first version, the critical difference lies in the pre-filtering step: Version 1 considers all events regardless of magnitude, while this version ensures that only significant events are used in the grouping. This approach is efficient and reduces the chance of including aftershocks by eliminating smaller events, but it still assumes that only one important event can occur each day, which could overlook closely timed mainshocks in seismically active regions. Overall, this method offers a practical balance between simplification and relevance by focusing on higher-magnitude data and applying a daily grouping strategy.
The Omori-Utsu law, also known as the modified Omori law, is a widely recognized empir- ical model in seismology that describes the temporal decay of aftershock activity following a main earthquake event. Initially proposed by Fusakichi Omori in 1894 and later gener- alized by Yoshiro Utsu, the law models how the frequency of aftershocks decreases over time. The mathematical formulation of the Omori-Utsu law is given by:
where:
This formulation was extensively studied and formalized in the work by Utsu in [5]:
Here we use Omori-Utsu law as a basis for clustering temporally related earthquake events, primarily to identify aftershock sequences. Rather than using the law to fit a time series, it is employed to determine whether two seismic events should be grouped into the same aftershock cluster.
For each earthquake event in a dataset, treated as a potential mainshock, the algo- rithm evaluates all subsequent events. The time difference t (in days) between the current event and each later event is calculated. The Omori-Utsu model is applied to estimate the expected rate of aftershocks at time t:
If n(t) exceeds a threshold, the subsequent event is assigned to the same cluster as the mainshock. This iterative clustering continues through all events in the dataset, assigning a unique identifier Occurrence No to each group.
After clustering, the mainshock of each group is identified as the event with the highest magnitude. The inter-arrival times between these mainshocks are then com- puted. Assuming that these main events follow a Poisson process, the code performs a Kolmogorov–Smirnov (KS) test to evaluate whether the inter-arrival times follow an exponential distribution, which is a key characteristic of a Poisson process.
Further we explored a grid of hyperparameter values for K, c, and p to determine the most appropriate clustering behavior for each file. The KS test is applied for each combi- nation of parameters, and the configuration that yields the highest p-value is considered the best-fitting model. The results are recorded and summarized across all datasets.
4.1 Basic Model
The results reveal that in 16 out of 29 states, the daily maximum magnitude events appear to follow a Poisson process, suggesting that in these regions, the occurrences of earthquakes are approximately random and independent over time. This is an important finding, as it supports the assumption of statistical regularity in seismicity in a majority of regions.
However, for the remaining 13 states, the data do not conform to the Poisson assump- tion. This deviation is likely due to the presence of aftershock sequences — clusters of events that occur shortly after a larger mainshock — which violate the independence assumption required for a Poisson model. Since this version of the model does not ex- plicitly remove or filter out aftershocks, such correlated events remain in the dataset and distort the temporal randomness expected in a Poisson process. Thus, while the basic model provides a useful first approximation, its limitations in accounting for aftershocks become evident in regions where clustered seismicity is more common.
|
State |
Lambda |
KS_P Value |
KS_Result |
|
Andaman and Nicobar island |
0.164025 |
0.015693 |
Does Not Fit Poisson |
|
Andhra Pradesh |
0.003003 |
0.968318 |
Fits Poisson |
|
Arunachal Pradesh |
0.132329 |
0.003378 |
Does Not Fit Poisson |
|
Assam |
0.064233 |
0.000359 |
Does Not Fit Poisson |
|
Chandigarh |
0.003903 |
0.845763 |
Fits Poisson |
|
Chhattisgarh |
0.015423 |
0.110945 |
Fits Poisson |
|
Gujarat |
0.046957 |
0.09279 |
Fits Poisson |
|
Haryana |
0.034734 |
0.009449 |
Does Not Fit Poisson |
|
Himachal Pradesh |
0.066819 |
0.001291 |
Does Not Fit Poisson |
|
Jammu and Kashmir |
0.081695 |
1.38E-05 |
Does Not Fit Poisson |
|
Karnataka |
0.013721 |
0.00095 |
Does Not Fit Poisson |
|
Madhya Pradesh |
0.004828 |
0.019326 |
Does Not Fit Poisson |
|
Maharashtra |
0.061265 |
8.62E-09 |
Does Not Fit Poisson |
|
Manipur |
0.128606 |
0.119707 |
Fits Poisson |
|
Meghalaya |
0.04897 |
0.023036 |
Does Not Fit Poisson |
|
Mizoram |
0.076343 |
0.209499 |
Fits Poisson |
|
Nagaland |
0.035244 |
0.346238 |
Fits Poisson |
|
Odisha |
0.00509 |
0.969141 |
Fits Poisson |
|
Punjab |
0.00937 |
0.694256 |
Fits Poisson |
|
Rajasthan |
0.034809 |
0.956175 |
Fits Poisson |
|
Sikkim |
0.051766 |
0.023483 |
Does Not Fit Poisson |
|
Tamil Nadu |
0.003752 |
0.074424 |
Fits Poisson |
|
Telangana |
0.012918 |
3.59E-08 |
Does Not Fit Poisson |
|
Uttar Pradesh |
0.009823 |
0.341248 |
Fits Poisson |
|
Kerala |
0.002824 |
0.648788 |
Fits Poisson |
|
Lakshadweep |
0.050568 |
0.005693 |
Does Not Fit Poisson |
|
New Delhi |
0.012628 |
0.73993 |
Fits Poisson |
|
Tripura |
0.01428 |
0.409838 |
Fits Poisson |
|
West Bengal |
0.009158 |
0.586967 |
Fits Poisson |
Table 1: Statewise Estmated Lambda and KS test result for Basic model
4.2 Clustered Model
When the Kolmogorov–Smirnov test is applied to this ”declustered” data, 14 out of 29 states show a good fit to the Poisson process. Although this is slightly fewer than the 16 states identified under the basic model, a notable outcome is that some states which previously failed the Poisson test in the basic model now pass it under the clustered approach. This indicates that for these states, the presence of tightly grouped aftershocks in the unfiltered dataset had previously masked the underlying randomness of mainshock events. Once the clustering is removed, the true Poisson-like behavior becomes apparent.
|
State |
Lambda |
KS PValue |
KS Result |
|
Andaman and Nicobar island |
0.055856 |
1.95E-08 |
Does Not Fit Poisson |
|
Arunachal Pradesh |
0.054996 |
1.32E-06 |
Does Not Fit Poisson |
|
Assam |
0.038757 |
6.71E-05 |
Does Not Fit Poisson |
|
Gujarat |
0.030011 |
0.005607 |
Does Not Fit Poisson |
|
Himachal Pradesh |
0.040256 |
0.000707 |
Does Not Fit Poisson |
|
Jammu and Kashmir |
0.041286 |
4.94E-05 |
Does Not Fit Poisson |
|
Karnataka |
0.010062 |
0.004096 |
Does Not Fit Poisson |
|
Madhya Pradesh |
0.004544 |
0.018161 |
Does Not Fit Poisson |
|
Maharashtra |
0.034409 |
0.002641 |
Does Not Fit Poisson |
|
Manipur |
0.061731 |
6.19E-13 |
Does Not Fit Poisson |
|
Meghalaya |
0.032217 |
0.002677 |
Does Not Fit Poisson |
|
Mizoram |
0.042546 |
1.85E-07 |
Does Not Fit Poisson |
|
Rajasthan |
0.026668 |
0.042704 |
Does Not Fit Poisson |
|
Sikkim |
0.031981 |
0.002619 |
Does Not Fit Poisson |
|
Telangana |
0.009982 |
1.83E-05 |
Does Not Fit Poisson |
|
Andhra Pradesh |
0.003003 |
0.968318 |
Fits Poisson |
|
Chandigarh |
0.003903 |
0.845763 |
Fits Poisson |
|
Chhattisgarh |
0.01428 |
0.13508 |
Fits Poisson |
|
Haryana |
0.025779 |
0.070784 |
Fits Poisson |
|
Nagaland |
0.026122 |
0.088345 |
Fits Poisson |
|
Odisha |
0.004525 |
0.864868 |
Fits Poisson |
|
Punjab |
0.008785 |
0.740547 |
Fits Poisson |
|
Tamil Nadu |
0.003439 |
0.100056 |
Fits Poisson |
|
Uttar Pradesh |
0.009004 |
0.534578 |
Fits Poisson |
|
Kerala |
0.0022 |
0.944968 |
Fits Poisson |
|
Lakshadweep |
0.01791 |
0.735759 |
Fits Poisson |
|
New Delhi |
0.011193 |
0.628538 |
Fits Poisson |
|
Tripura |
0.012083 |
0.844397 |
Fits Poisson |
|
West Bengal |
0.008608 |
0.510527 |
Fits Poisson |
Table 2: Statewise Estmated Lambda and KS test result for Clustered model
The slight decline in overall performance (from 16 to 14 states) suggests that while aftershock filtering improves the model in some regions, it might inadvertently eliminate meaningful independent events in others. Additionally, earthquakes with large magni- tudes tend to produce longer and more complex aftershock sequences, which are harder to separate from main events using simple clustering rules. This reflects the inconsistent nature of aftershocks, where their timing and frequency can vary significantly depending on the characteristics of the main event and local geology. Overall, this version represents a more sophisticated attempt to model earthquake occurrences by addressing the tempo- ral dependencies introduced by aftershocks. Though it slightly underperforms the basic model numerically, it provides a more realistic picture of independent seismic activity, especially in regions prone to clustering.
4.3 Truncated model
In the third approach, the modeling strategy is further refined by introducing a magnitude- based threshold to focus solely on larger and more impactful earthquakes. Specifically, only those seismic events with a magnitude greater than 5 are retained for analysis. This truncation serves two purposes: it filters out minor quakes that are more likely to be part of aftershock sequences or noise, and it concentrates on the mainshock events that are of greater geological and societal significance.
Following this magnitude thresholding, the dataset is further constrained by including only those states that have a sufficient number of qualifying observations—in this case, at least 5 events remaining after the truncation. As a result, only 10 states out of the original 29 meet this criterion and are carried forward into the modeling process.
For each of these selected states, the inter-arrival times of the filtered high-magnitude events are computed, and the Kolmogorov–Smirnov (K–S) test is applied to assess the goodness-of-fit to the Poisson process. The results are striking: all 9 states included in this filtered subset show inter-event times that are consistent with a Poisson distribution. This suggests that when we focus exclusively on higher-magnitude, well-separated events and exclude both low-magnitude events and states with sparse data, the assumption of Poisson-distributed earthquake occurrences becomes uniformly valid.
This version offers a tightly controlled and clean dataset, free from the clutter of minor quakes and short-term clustering. The uniformity of the results across the 10 states sug- gests that the Poisson process is a highly appropriate model for capturing the behavior of significant, independent seismic events. It highlights how proper filtering—both in terms of magnitude and data sufficiency—can lead to stronger and more consistent statistical conclusions.
The result obtained using the clustered model is given as follows.
|
State |
Lambda |
KS PValue |
KS Result |
|
Andaman and Nicobar island |
0.030776 |
0.07248 |
Fits Poisson |
|
Arunachal Pradesh |
0.010335 |
0.260183 |
Fits Poisson |
|
Gujarat |
0.003179 |
0.923036 |
Fits Poisson |
|
Jammu and Kashmir |
0.004267 |
0.566773 |
Fits Poisson |
|
Manipur |
0.004244 |
0.469809 |
Fits Poisson |
|
Mizoram |
0.004529 |
0.592703 |
Fits Poisson |
|
Rajasthan |
0.002062 |
0.722663 |
Fits Poisson |
|
Sikkim |
0.002949 |
0.917642 |
Fits Poisson |
|
Lakshadweep |
0.71614 |
0.291084 |
Fits Poisson |
Table 3: Statewise Estmated Lambda and KS test result for Truncated model
4.4 Ohmori-Utsu Model
After applying the Omori-Utsu clustering method with optimized hyperparameters across all 29 Indian states, it was observed that the inter-arrival times of the main earthquakes follow a Poisson process. This conclusion is supported by the Kolmogorov–Smirnov (KS) test, where each state’s dataset produced a p-value greater than the 0.05 threshold, indicating that the null hypothesis—that the inter-arrival times follow an exponential distribution—cannot be rejected. This result confirms that the method effectively isolates main shocks in a statistically consistent manner.
|
State |
K |
c |
p |
Lambda |
KS PValue |
KS Result |
|
Andaman and Nicobar island.csv |
2 |
0.1 |
0.9 |
0.003297 |
0.159952 |
Fits Poisson |
|
Andhra Pradesh |
0.5 |
0.1 |
1.3 |
0.003003 |
0.968318 |
Fits Poisson |
|
Arunachal Pradesh |
2 |
0.1 |
0.9 |
0.003058 |
0.063467 |
Fits Poisson |
|
Assam |
2 |
0.5 |
0.9 |
0.002818 |
0.198917 |
Fits Poisson |
|
Chandigarh |
0.5 |
0.1 |
1.1 |
0.003624 |
0.96883 |
Fits Poisson |
|
Chhattisgarh |
2 |
0.1 |
1.3 |
0.007534 |
0.771895 |
Fits Poisson |
|
Gujarat |
2 |
0.1 |
0.9 |
0.003014 |
0.235199 |
Fits Poisson |
|
Haryana |
2 |
0.1 |
0.9 |
0.003091 |
0.126379 |
Fits Poisson |
|
Himachal Pradesh |
1 |
0.1 |
0.9 |
0.005551 |
0.096574 |
Fits Poisson |
|
Jammu and Kashmir |
2 |
0.1 |
0.9 |
0.002994 |
0.168211 |
Fits Poisson |
|
Karnataka |
2 |
0.1 |
0.9 |
0.001843 |
0.928299 |
Fits Poisson |
|
Madhya Pradesh |
2 |
0.1 |
0.9 |
0.001455 |
0.99633 |
Fits Poisson |
|
Maharashtra |
2 |
0.1 |
0.9 |
0.00289 |
0.19997 |
Fits Poisson |
|
Manipur |
2 |
0.1 |
1.1 |
0.00798 |
0.087025 |
Fits Poisson |
|
Meghalaya |
2 |
0.1 |
0.9 |
0.002999 |
0.060053 |
Fits Poisson |
|
Mizoram |
2 |
0.1 |
0.9 |
0.003033 |
0.286631 |
Fits Poisson |
|
Nagaland |
2 |
0.1 |
0.9 |
0.003012 |
0.074088 |
Fits Poisson |
|
Odisha |
0.5 |
0.1 |
1.1 |
0.004242 |
0.727175 |
Fits Poisson |
|
Punjab |
0.5 |
0.1 |
1.3 |
0.007906 |
0.493958 |
Fits Poisson |
|
Rajasthan |
2 |
0.1 |
0.9 |
0.002931 |
0.121009 |
Fits Poisson |
|
Sikkim |
1 |
0.1 |
0.9 |
0.00559 |
0.357488 |
Fits Poisson |
|
Tamil Nadu |
2 |
0.1 |
1.1 |
0.002189 |
0.987978 |
Fits Poisson |
|
Telangana |
0.5 |
0.1 |
1.1 |
0.005625 |
0.756594 |
Fits Poisson |
|
Uttar Pradesh |
2 |
1 |
1.3 |
0.005812 |
0.465295 |
Fits Poisson |
|
Kerala |
0.5 |
0.1 |
0.9 |
0.001924 |
0.962501 |
Fits Poisson |
|
Lakshadweep |
0.5 |
0.1 |
0.9 |
0.01791 |
0.735759 |
Fits Poisson |
|
New Delhi |
0.5 |
1 |
1.3 |
0.010045 |
0.43517 |
Fits Poisson |
|
Tripura |
0.5 |
0.5 |
1.3 |
0.010479 |
0.279583 |
Fits Poisson |
|
West Bengal |
0.5 |
1 |
1.3 |
0.007775 |
0.412087 |
Fits Poisson |
Table 4: Statewise Estmated Lambda and KS test result for Ohmori-Utsu model
Compared to the basic static clustering model, which uses fixed temporal or spatial windows to group earthquake events, the Omori-Utsu approach offers significant improve- ments. Static clustering does not adapt to local variations in aftershock decay, which can result in either over-clustering or missing key seismic events. In contrast, the Omori- Utsu model dynamically clusters events using a time-dependent decay law defined by the equation:
where the parameters K, c, and p control the aftershock rate. This approach allows clustering to adjust based on seismicity characteristics specific to each state, leading to more accurate identification of main shocks.
The method also outperforms truncation-based models that classify earthquakes based on a magnitude threshold. Such models assume that only high-magnitude events can be main shocks, which can result in the exclusion of significant lower-magnitude main events, especially in seismically quieter regions. The Omori-based model avoids this bias by considering the temporal relationships between events rather than magnitude alone. This inclusivity ensures that relevant events are retained for analysis and that the derived inter-arrival times more accurately reflect the true underlying process.
Finally, the validation of the model using the Kolmogorov–Smirnov test across all states demonstrates the effectiveness of the Omori-Utsu clustering in extracting a main shock sequence that adheres to the assumptions of a Poisson process. This consistency across diverse seismic environments in India shows the robustness of the method and its potential for use in reliable seismic hazard assessment.
CONCLUSION
This study illustrates the complexities inherent in modeling earthquake occurrences across Indian states. While the Poisson process and subsequent models provide valuable frame- works for understanding seismic behavior, our findings indicate that careful consideration of aftershocks and event magnitudes is critical for accurate representation. The analysis demonstrated that regions exhibiting significant aftershock activity may require tailored approaches to capture the dynamics of seismic events effectively.
The success of the Omori-Utsu model in fitting all states reinforces the importance of adapting modeling techniques to account for temporal decay patterns. Moving forward, it is essential to explore non-Poissonian models and integrate spatial data to enhance predictive accuracy and better inform seismic risk assessments. By developing more so- phisticated and region-specific modeling strategies, we can improve our understanding of earthquake behavior and contribute to more effective disaster preparedness and mitiga- tion efforts.
REFERENCES
Sathyala Suresh*, Navaneeth V., Sona Mathew, Tirupathi Rao Padi, Prevalence Of Earthquake Prediction With Reference To Indian Geographical States Through Data Insights, Int. J. Sci. R. Tech., 2026, 3 (7), 795-804. https://doi.org/10.5281/zenodo.21530234
10.5281/zenodo.21530234