In this article, we propose a kind of numerical methods based on the Padé approxi
mations, for two kinds of stochastic Hamiltonian systems. For the general linear stochastic Hamiltonian systems, it is shown that the applied Padé approxi
mations
mathmlsrc">mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0377042716303715&_mathId=si1.gif&_user=111111111&_pii=S0377042716303715&_rdoc=1&_issn=03770427&md5=b7bc20ec7362aea9208e13acd15aedba" title="Click to view the MathML source">P(k,k)mathContainer hidden">mathCode"><math altimg="si1.gif" overflow="scroll">P(k,k)math> produce numerical solutions that are symplectic, and the proposed numerical schemes based on
mathmlsrc">mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0377042716303715&_mathId=si2.gif&_user=111111111&_pii=S0377042716303715&_rdoc=1&_issn=03770427&md5=c2c2d5d19f9727bbcdc39242a27d806e" title="Click to view the MathML source">P(r,s)mathContainer hidden">mathCode"><math altimg="si2.gif" overflow="scroll">P(r,s)math> are of root-mean-square convergence order
mathmlsrc">mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0377042716303715&_mathId=si3.gif&_user=111111111&_pii=S0377042716303715&_rdoc=1&_issn=03770427&md5=d468e31eb6b8c63f3e0592d5261109d4">
mage" height="19" width="21" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0377042716303715-si3.gif">mathContainer hidden">mathCode"><math altimg="si3.gif" overflow="scroll">r+s2math>. For a special kind of linear stochastic Hamiltonian systems with additive noises, the numerical methods using two kinds of Padé approxi
mations,
mathmlsrc">mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0377042716303715&_mathId=si4.gif&_user=111111111&_pii=S0377042716303715&_rdoc=1&_issn=03770427&md5=a2af92b2fee57c67d6d683cc09dc86b7">
mage" height="17" width="31" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0377042716303715-si4.gif">mathContainer hidden">mathCode"><math altimg="si4.gif" overflow="scroll">P(rˆ,sˆ)math> and
mathmlsrc">mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0377042716303715&_mathId=si5.gif&_user=111111111&_pii=S0377042716303715&_rdoc=1&_issn=03770427&md5=38ad848c5d42e082f6978a94c15f8d73">
mage" height="17" width="33" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0377042716303715-si5.gif">mathContainer hidden">mathCode"><math altimg="si5.gif" overflow="scroll">P(ř,1)math>, possess root-mean-square convergence order
mathmlsrc">mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0377042716303715&_mathId=si6.gif&_user=111111111&_pii=S0377042716303715&_rdoc=1&_issn=03770427&md5=f9ed9319cf9d189387ebd05e874a3b1b">
mage" height="13" width="37" alt="View the MathML source" style="margin-top: -5px; vertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0377042716303715-si6.gif">mathContainer hidden">mathCode"><math altimg="si6.gif" overflow="scroll">ř+2math> when
mathmlsrc">mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0377042716303715&_mathId=si7.gif&_user=111111111&_pii=S0377042716303715&_rdoc=1&_issn=03770427&md5=0445a13bdd0d78e4980f3dc7b6c9753b">
mage" height="13" width="93" alt="View the MathML source" style="margin-top: -5px; vertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0377042716303715-si7.gif">mathContainer hidden">mathCode"><math altimg="si7.gif" overflow="scroll">rˆ+sˆ=ř+3math>, and are symplectic if
mathmlsrc">mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0377042716303715&_mathId=si8.gif&_user=111111111&_pii=S0377042716303715&_rdoc=1&_issn=03770427&md5=5c3e8d5aec19a42e31ae43d87a9ef353">
mage" height="12" width="37" alt="View the MathML source" style="margin-top: -5px; vertical-align: middle" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0377042716303715-si8.gif">mathContainer hidden">mathCode"><math altimg="si8.gif" overflow="scroll">rˆ=sˆmath>. These generalize the Padé approxi
mation approaches for symplectic integration of linear Hamiltonian systems to the stochastic context.