Exact e – e (exchange) correlations of 2-D quantum dots in magnetic field: Size extensiveN=3,4,…,′n′-electron systems via multi-pole expansion

2017 ◽  
Vol 88 ◽  
pp. 26-34 ◽  
Author(s):  
Priyanka Aggarwal ◽  
Shivalika Sharma ◽  
Sunny Singh ◽  
Harsimran Kaur ◽  
Ram Kuntal Hazra
ACS Omega ◽  
2017 ◽  
Vol 2 (10) ◽  
pp. 7410-7423 ◽  
Author(s):  
Harsimran Kaur ◽  
Sunny Singh ◽  
Priyanka Aggarwal ◽  
Shivalika Sharma ◽  
Sambhav Yadav ◽  
...  

Entropy ◽  
2018 ◽  
Vol 20 (8) ◽  
pp. 557 ◽  
Author(s):  
Oscar Negrete ◽  
Francisco Peña ◽  
Juan Florez ◽  
Patricio Vargas

In this work, we report the magnetocaloric effect (MCE) in two systems of non-interactive particles: the first corresponds to the Landau problem case and the second the case of an electron in a quantum dot subjected to a parabolic confinement potential. In the first scenario, we realize that the effect is totally different from what happens when the degeneracy of a single electron confined in a magnetic field is not taken into account. In particular, when the degeneracy of the system is negligible, the magnetocaloric effect cools the system, while in the other case, when the degeneracy is strong, the system heats up. For the second case, we study the competition between the characteristic frequency of the potential trap and the cyclotron frequency to find the optimal region that maximizes the ΔT of the magnetocaloric effect, and due to the strong degeneracy of this problem, the results are in coherence with those obtained for the Landau problem. Finally, we consider the case of a transition from a normal MCE to an inverse one and back to normal as a function of temperature. This is due to the competition between the diamagnetic and paramagnetic response when the electron spin in the formulation is included.


1990 ◽  
Vol 216 ◽  
Author(s):  
Kamakhya P. Ghatak ◽  
S. N. Biswas

ABSTRACTIn this paper we studied the thermoelectric power under classically large magnetic field (TPM) in quantum wells (QWs), quantum well wires (QWWS) and quantum dots (QDs) of Bi by formulating the respective electron dispersion laws. The TPM increases with increasing film thickness in an oscillatory manner in all the cases. The TPM in QD is greatest and the least for quantum wells respectively. The theoretical results are in agreement with the experimental observations as reported elsewhere.


2006 ◽  
Vol 119-120 ◽  
pp. 565-569 ◽  
Author(s):  
F. Saito ◽  
M. Yamagiwa ◽  
K. Ikeda ◽  
Y. Ogawa ◽  
F. Minami ◽  
...  
Keyword(s):  

2002 ◽  
Vol 66 (23) ◽  
Author(s):  
I. A. Yugova ◽  
I. Ya. Gerlovin ◽  
V. G. Davydov ◽  
I. V. Ignatiev ◽  
I. E. Kozin ◽  
...  

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