A birth-death chain on has generator entries , for , , , and zero elsewhere. Assume the usual conservative nonexplosive chain. The detailed balance for a birth-death process are .
If they hold, each incoming term cancels an outgoing term, giving and thus invariance. Conversely the invariance equation at zero gives . At state , write the stationarity equation as equality of the neighbouring probability currentsInduction from the zero boundary current gives detailed balance for a birth-death process for every edge. Thus invariant measures are exactly the detailed-balance measures in this standard birth–death setting. The argument is the generator characterization; a stationary probability law additionally needs finite normalization. For potentially explosive processes, formal generator balance alone would require additional boundary qualifications.
The number present is an M-M-s queue: births occur at rate , deaths at rate . Both rates are bounded, so the chain is nonexplosive. For and an integer , the detailed-balance weights with areTheir sum is finite precisely when , giving positive recurrence and a stationary probability distribution after normalization.
For completeness, the birth–death recurrence criterion is . It follows by solving the harmonic hitting-probability recurrence: successive differences are proportional to , and divergence makes the probability of escaping to infinity before reaching zero vanish. The geometric tail of the weights makes this sum diverge when and converge when . Thus gives null recurrence, since the chain is recurrent but has no finite invariant normalization, and gives transience. The critical case is not positive recurrent merely because arrival and maximum service rates balance.
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