68 Hidden Markov Models
Every clustering technique in the previous topic treated observations as independent of each other: farm 7’s cluster assignment had nothing to do with farm 6’s. Hidden Markov Models (Lawrence R. Rabiner, 1989) handle a different situation, one where order matters: a sequence of observations collected over time from the same subject, where the thing generating those observations is itself changing state as time passes, and that underlying state is never observed directly.
A field’s disease condition is a natural example. Nobody directly observes “this field entered a stressed state in week 4.” What gets observed instead is a proxy, a satellite NDVI reading, a visible symptom score, and the true underlying condition, the hidden state, has to be inferred from that sequence of indirect, imperfect observations. That is exactly the problem a Hidden Markov Model is built to solve.
68.2 Worked Example
One field, tracked weekly over a ten-week stretch of the growing season. The hidden state each week is the field’s true condition, Healthy or Stressed, never observed directly. What is observed is a weekly NDVI reading, bucketed into Low, Medium, or High. The model’s known parameters, estimated from historical data on similar fields, are given below.
Initial state distribution (\(\pi\)): Healthy 0.70, Stressed 0.30 (most fields start the season healthy).
Transition matrix (\(A\)):
| From \ To | Healthy | Stressed |
|---|---|---|
| Healthy | 0.85 | 0.15 |
| Stressed | 0.25 | 0.75 |
Emission matrix (\(B\)):
| State | Low NDVI | Medium NDVI | High NDVI |
|---|---|---|---|
| Healthy | 0.10 | 0.30 | 0.60 |
| Stressed | 0.60 | 0.30 | 0.10 |
Observed sequence, weeks 1 through 10: High, High, Medium, Low, Low, Low, Medium, High, High, High.
68.4 Reading the Result
The decoded state sequence should track the observed NDVI pattern closely but not identically: the model is weighing both the emission probabilities (how likely each NDVI reading is under each state) and the transition probabilities (how likely the field is to have actually switched states between two consecutive weeks), so an isolated one-week dip that would be cheap to explain as noise under a state that persisted may get smoothed over rather than triggering an immediate state switch. That smoothing is the entire value the Markov structure adds over simply thresholding each week’s NDVI reading in isolation: it uses the whole sequence, not just the current reading, to decide what state a field was most likely in during any given week. The probability of the sequence itself is a much smaller number than it might look, an inescapable consequence of multiplying ten separate probabilities together, and it is far more useful for comparing two candidate sequences or two candidate models against each other than for interpreting on its own.
Summary
| Concept | Description |
|---|---|
| Foundations | |
| Hidden Markov Model | Infers an unobserved underlying state from a sequence of indirect, imperfect observations over time |
| Hidden States and the Markov Property | The next hidden state depends only on the current state, not the full history of states before it |
| Transition Matrix | Gives the probability of moving from each hidden state to each other state at the next time step |
| Emission Matrix | Gives the probability of each possible observed signal, given the current hidden state |
| Worked Example | |
| Worked Example: Ten Weeks of NDVI Readings | A field's true weekly condition, Healthy or Stressed, inferred from ten weeks of bucketed NDVI readings |
| The Viterbi Algorithm | Decodes the single most likely hidden state sequence given an observed sequence and the model parameters |
| The Forward Algorithm | Computes the total probability of an observed sequence under the model, useful for comparing sequences or models |
| Why the Full Sequence Matters | Weighing the whole sequence, not just one reading at a time, smooths over noise a single-week threshold would miss |