2019
DOI: 10.1007/s11071-019-05001-w
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Analyzing the geometric phase for self-oscillations in field emission nanowire mechanical resonators

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Cited by 4 publications
(2 citation statements)
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“…In many cases, it enables us to derive quantum solutions of TDHSs. [ 31–34 ] From the Liouville‐von Neumann equation, normaldtrueÎ/normaldt=trueÎ/t+(i)1false[trueÎ,Ĥqfalse]=0, we can establish a linear invariant operator [ 31 ] of the system such that Î=cX(t)[p̂pnormalpfalse(tfalse)]iscriptA(t)[x̂xnormalpfalse(tfalse)]eiη(t)where c is a complex constant, pnormalpfalse(tfalse) is a particular solution of the classical equation of motion of the system in momentum space, Xfalse(tfalse)=X12false(tfalse)+X22false(tfalse), and truerightscriptAfalse(tfalse)=leftΩXfalse(tfalse)imexpq(βt)trueẊ(t) truerightηfalse(tfalse)=leftΩm0tdtX2...…”
Section: Resultsmentioning
confidence: 99%
“…In many cases, it enables us to derive quantum solutions of TDHSs. [ 31–34 ] From the Liouville‐von Neumann equation, normaldtrueÎ/normaldt=trueÎ/t+(i)1false[trueÎ,Ĥqfalse]=0, we can establish a linear invariant operator [ 31 ] of the system such that Î=cX(t)[p̂pnormalpfalse(tfalse)]iscriptA(t)[x̂xnormalpfalse(tfalse)]eiη(t)where c is a complex constant, pnormalpfalse(tfalse) is a particular solution of the classical equation of motion of the system in momentum space, Xfalse(tfalse)=X12false(tfalse)+X22false(tfalse), and truerightscriptAfalse(tfalse)=leftΩXfalse(tfalse)imexpq(βt)trueẊ(t) truerightηfalse(tfalse)=leftΩm0tdtX2...…”
Section: Resultsmentioning
confidence: 99%
“…For more recent advancements in quantum learning, please refer to [35,[37][38][39][40][41][42][43][44][45][46][47][48][49]. These studies highlight the latest developments in this rapidly evolving field.…”
Section: Quantum Mechanics Based On Machine Learningmentioning
confidence: 99%