ProofComplete

Proof of ItΓ΄ Isometry

We prove E[(∫0THt dBt)2]=E[∫0THt2 dt]\mathbb{E}[(\int_0^T H_t \, dB_t)^2] = \mathbb{E}[\int_0^T H_t^2 \, dt] for simple processes, then extend by density.

Step 1: For simple Ht=βˆ‘i=0nβˆ’1Hi1[ti,ti+1)H_t = \sum_{i=0}^{n-1} H_i \mathbf{1}_{[t_i, t_{i+1})}, expand the square:

(∫0THt dBt)2=(βˆ‘iHiΞ”Bi)2=βˆ‘iHi2(Ξ”Bi)2+2βˆ‘i<jHiHjΞ”BiΞ”Bj.\left(\int_0^T H_t \, dB_t\right)^2 = \left(\sum_i H_i \Delta B_i\right)^2 = \sum_i H_i^2 (\Delta B_i)^2 + 2\sum_{i<j} H_i H_j \Delta B_i \Delta B_j.

Step 2: Take expectations. The cross terms vanish by independence: E[HiHjΔBiΔBj]=E[HiHj]E[ΔBi]E[ΔBj]=0\mathbb{E}[H_i H_j \Delta B_i \Delta B_j] = \mathbb{E}[H_i H_j] \mathbb{E}[\Delta B_i] \mathbb{E}[\Delta B_j] = 0 for i≠ji \neq j.

Step 3: For the diagonal terms: E[Hi2(Ξ”Bi)2]=E[Hi2](ti+1βˆ’ti)\mathbb{E}[H_i^2 (\Delta B_i)^2] = \mathbb{E}[H_i^2] (t_{i+1} - t_i).

Summing over ii gives the isometry. Extension to general L2L^2 processes follows by approximation and continuity of the L2L^2 norm.