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Merge pull request #52 from jstac/ucms
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ucms1_typos1
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jstac authored Oct 7, 2020
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8 changes: 4 additions & 4 deletions ctmc_lectures/uc_mc_semigroups.md
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Expand Up @@ -35,7 +35,7 @@ The main aim is to give an exact one-to-one correspondence between
Conservativeness is defined below and relates to "nonexplosiveness" of the
associated Markov chain.

We will also give a brief discussion of intensity matricies that do not have
We will also give a brief discussion of intensity matrices that do not have
this property, along with the processes they generate.


Expand Down Expand Up @@ -249,7 +249,7 @@ $t \geq 0$ and $Q$ is the generator of $(P_t)$, with $P_0' = Q$.
Our definition of a conservative intensity matrix works for the theory above
but can be hard to check in appliations and lacks probabilistic intuition.
Fortunately, we have the following simple charcterization.
Fortunately, we have the following simple characterization.
```{proof:lemma}
Expand Down Expand Up @@ -360,7 +360,7 @@ As we now show, every intensity matrix admits the decomposition in
### Jump Chain Decomposition
Given a intensity matrix $Q$, set
Given an intensity matrix $Q$, set
$$
\lambda(x) := -Q(x, x)
Expand Down Expand Up @@ -453,7 +453,7 @@ this produces a Markov chain with Markov semigroup
$(P_t)$ where $P_t = e^{tQ}$ for $Q$ satisfying {eq}`jcinmat`.
(Although our argument assumed finite $S$, the proof goes through when
$S$ is contably infinite and $Q$ is conservative with very minor changes.)
$S$ is countably infinite and $Q$ is conservative with very minor changes.)
In particular, $(X_t)$ is a continuous time Markov chain with intensity matrix
$Q$.
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