2015
DOI: 10.4208/cicp.110914.281014a
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The Split-Operator Technique for the Study of Spinorial Wavepacket Dynamics

Abstract: Abstract. The split-operator technique for wave packet propagation in quantum systems is expanded here to the case of propagating wave functions describing Schrödinger particles, namely, charge carriers in semiconductor nanostructures within the effective mass approximation, in the presence of Zeeman effect, as well as of Rashba and Dresselhaus spin-orbit interactions. We also demonstrate that simple modifications to the expanded technique allow us to calculate the time evolution of wave packets describing Dir… Show more

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Cited by 36 publications
(35 citation statements)
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References 38 publications
(46 reference statements)
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“…Alternatively, as we are interested only in the trion ground state, we obtain it by evolving an arbitrary initial wave packet in imaginary time τ = it until convergence is reached. The potential and kinetic energy terms in the time evolution operator U (τ + τ, τ ) = exp(−H ± τ/h) are conveniently split into a series of exponentials [51][52][53], where T i is the kinetic energy term in the i direction (for a system with N dimensions). This procedure requires lower computational cost, by paying the price of having a O( τ 3 ) error due to the noncommutativity between kinetic and potential operators, which is controlled here by using a small imaginary time step τ .…”
Section: B Neutral and Charged Excitonsmentioning
confidence: 99%
“…Alternatively, as we are interested only in the trion ground state, we obtain it by evolving an arbitrary initial wave packet in imaginary time τ = it until convergence is reached. The potential and kinetic energy terms in the time evolution operator U (τ + τ, τ ) = exp(−H ± τ/h) are conveniently split into a series of exponentials [51][52][53], where T i is the kinetic energy term in the i direction (for a system with N dimensions). This procedure requires lower computational cost, by paying the price of having a O( τ 3 ) error due to the noncommutativity between kinetic and potential operators, which is controlled here by using a small imaginary time step τ .…”
Section: B Neutral and Charged Excitonsmentioning
confidence: 99%
“…This approximation, based on the Suzuki-Trotter expansion, has a O(∆τ 3 ) error, which is controlled here by using a small imaginary timestep ∆τ . [29][30][31] By propagating an arbitrary initial wave function in imaginary time, this method directly yields the trion ground state energy E T and the trion wave function, but requires storing a high-dimensional numerical array. In this case, reducing the number of variables of the system is of essence.…”
mentioning
confidence: 99%
“…This value is determined by condition (50), which implies that a typical anomalous velocity induced by SOC, V so ∼ α, exceed the collapse velocity V c , see Eq. (32). If α = α cr , the simulations demonstrate that the BEC starts its evolution by compressing in the beginning, but then slightly expands (not shown in detail).…”
Section: Collapse In the Presence Of The Spin-orbit Coupling And mentioning
confidence: 89%