Type a command or search the notes. Tab cycles completions. Up and down recall history when blank. Escape dismisses, then leaves the prompt.
MATH
[1251]

Proofs from Markov systems

All proofs from Markov systems.

Back to Markov systems

Non-negativity follows because each entry of AxA\mathbf{x} is a sum of products of non-negative numbers. Let 1\mathbf{1} be the all-ones vector. Since the columns of AA sum to 11,

1TA=1T.\mathbf{1}^{\mathsf T}A=\mathbf{1}^{\mathsf T}.

Therefore

1TAx=1Tx=1.\mathbf{1}^{\mathsf T}A\mathbf{x} =\mathbf{1}^{\mathsf T}\mathbf{x} =1.

The column-sum condition gives

AT1=1,A^{\mathsf T}\mathbf{1}=\mathbf{1},

so 11 is an eigenvalue of ATA^{\mathsf T}. Since

det⁡(AT−λI)=det⁡((A−λI)T)=det⁡(A−λI),\det(A^{\mathsf T}-\lambda I) =\det\bigl((A-\lambda I)^{\mathsf T}\bigr) =\det(A-\lambda I),

AA and ATA^{\mathsf T} have the same eigenvalues. Hence 11 is an eigenvalue of AA. The all-ones vector is generally an eigenvector of ATA^{\mathsf T}, not of AA.

Let v1,…,vnv_1,\ldots,v_n be an eigenbasis with Av1=v1Av_1=v_1 and Avj=λjvjAv_j=\lambda_jv_j for j≥2j\ge2. Expand the initial state as

x(0)=α1v1+⋯+αnvn.\mathbf{x}(0)=\alpha_1v_1+\cdots+\alpha_nv_n.

Repeated application of AA gives

x(k)=Akx(0)=α1v1+∑j=2nαjλjkvj.\mathbf{x}(k)=A^k\mathbf{x}(0) =\alpha_1v_1+\sum_{j=2}^n\alpha_j\lambda_j^kv_j.

Since ∣λj∣<1|\lambda_j|<1 for j≥2j\ge2, the sum tends to zero. Thus x(k)→α1v1\mathbf{x}(k)\to\alpha_1v_1. For j≥2j\ge2, the column-sum identity 1TA=1T\mathbf1^{\mathsf T}A=\mathbf1^{\mathsf T} gives 1Tvj=λj1Tvj\mathbf1^{\mathsf T}v_j=\lambda_j\mathbf1^{\mathsf T}v_j, hence 1Tvj=0\mathbf1^{\mathsf T}v_j=0. Since the eigenvectors form a basis, v1v_1 must have non-zero component sum. The preserved initial sum therefore determines α1v1\alpha_1v_1 uniquely. If the initial state is a probability vector, every x(k)\mathbf{x}(k) is one too, so its limit is non-negative and sums to 11.