Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Springer eBooks

Towards a theory of noncommutative semimartingales adapted to Brownian motion and a quantum Ito's formula

R. L. Hudson, Rajeeva Laxman Karandikar, Kalyanapuram Rangachari Parthasarathy

Published Jan 31, 2006• 10 citations
Publisher
DOI
10.1007/bfb0044684

Related papers

Functional Ito Formula for Quantum Semimartingales (Infinite Dimensional Analysis and Quantum Probability Theory)

Un Cig Ji

数理解析研究所講究録•Aug 1, 2001•0 citations

Decoherence of quantum Brownian motion in noncommutative space

Sayed Ali Akbar Ghorashi, M. Bagheri Harouni

Physics Letters A•Feb 13, 2013•11 citations

On the theory of quantum brownian motion

R.F Roose, R. Dagonnier

Physica•Feb 1, 1972•0 citations

Nonlinear Theory of Quantum Brownian Motion

Roumen Tsekov

arXiv:0711.1442•International Journal of Theoretical Physics•Jul 8, 2008•14 citations

The Ito Formula for Perturbed Brownian Martingales

G. F. Vincent-Smith

In a further generalisation of the classical Ito formula, we show that if B = ( A t + A t † : t ∈ ] 0 , 1 [ ) is the Brownian quantum martingale and J = (Jt: t ∈ [0, 1]) is a bounded quantum semimartingale, then M = (Bt Jt: t ∈ [0, 1]) satisfies the functional quantum Ito formula [10, Section 6] [formula] The proof, which relies on the classical theory of unbounded self-adjoint operators, may be adapted to the case where B is replaced by a classical Brownian martingale. 2000 Mathematics Subject Classification 81S25, 60J65, 47D03.

Bulletin of the London Mathematical Society•Nov 1, 2000•3 citations

Stochastic integral representation theorem for quantum semimartingales

Un Cig Ji

Journal of Functional Analysis•May 19, 2003•23 citations
In a further generalisation of the classical Ito formula, we show that if B = ( A t + A t † : t ∈ ] 0 , 1 [ ) is the Brownian quantum martingale and J = (Jt: t ∈ [0, 1]) is a bounded quantum semimartingale, then M = (Bt Jt: t ∈ [0, 1]) satisfies the functional quantum Ito formula [10, Section 6] [formula] The proof, which relies on the classical theory of unbounded self-adjoint operators, may be adapted to the case where B is replaced by a classical Brownian martingale. 2000 Mathematics Subject Classification 81S25, 60J65, 47D03.